Kinematic Unification of Gravitational and Electromagnetic Phenomena
Jody A. Geiger
Informativity Institute
Chicago, IL USA 60605
jodygeiger@informativity.org
ORCID: 0000–0001–5389–0447
ABSTRACT
We present Measurement Quantization (MQ) as a count-based kinematic framework in which physical observables arise from discrete Internal Frame measure and are realized through the Frames mapping into the System Frame. Within this formulation, electromagnetic and gravitational phenomena emerge from count-dependent realizations of a single action defined over integer measure counts, with continuum field descriptions recovered through coarse-graining. MQ reproduces relativistic and gauge invariant structures while introducing a frame dependent non-Lorentz length contraction governed by the Informativity differential 2QLnL, which modifies normalization of inferred quantities as a function of count separation. Across established benchmarks, MQ yields quantitative concordance with experiment at a cumulative significance of 8.74σ, with independent cross-channel tests exceeding 5σ and CODATA consistency achieved at the 3.94σ level for a common observable. Notably, the evolution of CODATA values for the gravitational constant aligns with distinct MQ realizations at residuals well below reported experimental uncertainties, consistent with shifts in statistically dominant measurement scales. MQ further yields closed-form relations linking electromagnetic and gravitational observables, including distinct finite-count and asymptotic realizations of G, and reduces all coupling constants to functions of fundamental measures and the invariant scalar θsi, eliminating independent coupling parameters. Unlike conventional unification approaches based on symmetry extension or geometric postulates, MQ derives both geometry and interaction strength from a shared discrete kinematic origin. The framework is experimentally falsifiable through cross-channel comparisons of inferred quantities and predicted count-dependent normalization effects. These results establish MQ as a quantitatively constrained unification candidate grounded in first principles measure structure.
Keywords: Measurement Quantization, unification, gravity, electromagnetism, fundamental units, foundations of physics
1. INTRODUCTION
The objective of unification has historically been to demonstrate that apparently distinct physical interactions arise from a single underlying structure. In its strongest form, unification requires not only formal compatibility between theories, but the elimination of independent postulates, parameters, and sector-specific assumptions. The persistence of multiple interaction frameworks – most notably gravitation and electromagnetism – indicates that such a reduction has not yet been achieved within the standard theoretical paradigm.
This work approaches the unification problem from a strictly kinematic standpoint. Rather than beginning with fields, forces, or geometric curvature as primitives, it adopts a count-based description of physical separation and interaction. The implications of this shift are developed in subsequent sections. Here, we restrict attention to the historical development of the unification problem and the structural obstruction that has prevented its resolution.
1.1 The Unification Problem
The unification of physical interactions has been a central objective of theoretical physics since the nineteenth century. The first successful unification was achieved by Maxwell, who demonstrated that electricity and magnetism are manifestations of a single electromagnetic field described by a unified set of differential equations [1]. This result established a paradigm: distinct phenomena could be understood as different realizations of a single underlying structure.
The next major advance occurred with Einstein’s formulation of General Relativity (GR), in which gravitation is not treated as a force but as curvature of spacetime induced by energy–momentum [2]. While conceptually profound, this formulation introduced a structural divergence from electromagnetism. Electromagnetism is described as a gauge theory on a fixed spacetime background, whereas gravitation defines the geometry of spacetime itself. This distinction – geometric versus field-theoretic description – has remained a central barrier to unification.
Early attempts to bridge this divide focused on geometric extensions. The Kaluza–Klein framework introduced higher-dimensional spacetime in which electromagnetic degrees of freedom emerge from metric components [3,4]. Although elegant, these models required additional dimensions without empirical necessity and did not eliminate independent coupling structures. Later developments in gauge theory, particularly Yang–Mills theory, generalized the electromagnetic U(1) symmetry to non-Abelian groups, forming the basis of the Standard Model [5]. However, gravity remained external to this framework.
Efforts to incorporate gravity into a unified quantum framework led to string theory and related approaches, in which all interactions arise from excitations of fundamental extended objects [6,7]. While these theories achieve formal unification at high energies, they introduce a vast landscape of possible solutions and rely on structures not directly accessible to experiment. Loop quantum gravity and other non-perturbative approaches attempt to quantize spacetime itself [8], but do not unify gravity with the gauge interactions in a single dynamical object.
Across these approaches, a common pattern emerges: unification is pursued by adding structure – extra dimensions, additional symmetries, new fields, or quantization prescriptions. This strategy has achieved partial success but has not eliminated the fundamental separation between interaction sectors. In particular, independent coupling constants (e.g. e, G, ℏ) persist, distinct mathematical frameworks are retained for different interactions and the origin of these structures is not derived from a single primitive. This persistent separation suggests that the obstruction to unification is not merely technical, but conceptual.
1.1.1 Structural Obstruction in Classical and Modern Frameworks
The central obstruction can be stated as follows. Existing theories assume continuum primitives – fields, metrics, or wave functions – defined on a pre-existing manifold. Within this assumption, geometry (GR) and gauge structure (EM/SM) arise from different foundational objects. Couplings are introduced and phenomenologically, discrete physical measurement plays no fundamental role in defining structure.
Because these primitives are assumed rather than derived, attempts at unification must reconcile incompatible starting points. The result is either hybrid theories (GR + quantum field theory) or extended frameworks that preserve the underlying separation.
1.1.2 MQ Perspective: Bypassing the Obstruction
Measurement Quantization (MQ) departs from this paradigm by removing continuum primitives from the foundation of the theory. Instead, it begins with integer counts of fundamental measures ([9], Appx. W), from which both geometry and field behavior emerge. In this framework, spatial and temporal separations are defined by counts nL and nT, The invariant ratio c = lf/tf establishes relativistic structure without postulating spacetime geometry, and continuum descriptions arise only as coarse-grained representations of an underlying discrete count structure.
The key implication is that geometry and interaction are no longer distinct constructs. Both are consequences of the same Frames mapping between the Internal Frame and System Frame, as defined in the MQ formalism (see Appx. A) ([9], Appx. K). This shift bypasses the historical obstruction. No independent metric is assumed. That is, gravitational structure emerges from a common count geometry ([9], Appx. I, J). No independent gauge field is introduced. Rather, electromagnetic behavior emerges as a symmetry of count relabeling. And no separate coupling constants are required. Instead, interaction strengths derive from a single geometric scalar ([9], Appx. P,Q,AA). In this way, MQ does not unify existing theories by embedding them in a larger structure. Instead, it replaces their foundational assumptions, allowing both gravitational and electromagnetic phenomena to arise from a common kinematic origin.
1.2 MQ as a Count–Based Kinematic Framework
This section introduces the minimal structure required to define MQ, with emphasis on the geometric interpretation of the Frames Principle. We will gain an understanding of this principle through the right–triangle construction provided in Fig. 1.
First, the Frames Principle asserts that all physically meaningful measures arise from mappings between a discrete Internal Frame defined by integer count structure and a non-discrete System Frame. A frame is understood as a self-consistent realization of fundamental measures – length, time, and interaction – constructed from countable units within a configuration domain. Physical observables do not exist in isolation, but only as relational quantities established through admissible mappings between such frames. These mappings preserve invariant couplings while permitting systematic deformation in measured quantities, a property of the underlying discrete geometry. In this way, apparent continuous symmetries emerge as large-scale limits of count-preserving transformations, and geometric relations – such as the right–triangle construction introduced below – serve as the minimal representation of consistency between frames.
1.2.1 Fundamental Counts and Invariant Ratio
MQ begins with two primary quantities: the integer counts nL and nT, representing separations in units of the fundamental length lf and fundamental time tf, respectively. These counts define a discrete kinematic structure in which physical distance and duration are not continuous primitives but are constructed from countable units.
The invariant relation between these counts is given by c = lf/tf, where c is the invariant conversion factor linking temporal and spatial counts. Let ω denote the Internal Frame configuration domain and let ω′ be a relational region over which counts are defined. Physical realization proceeds through a mapping , where ℛ is the emergent System Frame relational structure in which geometric observables are defined. See Appx. A for formal definitions of all symbols.
This relation does not arise as an imposed postulate, but as a closure constraint required for mapping consistency. A fixed ratio lf/tf is the unique condition under which count-based transformations between temporal and spatial separations remain single-valued, independent of the sequence of count operations. Equivalently, admissible mappings must commute under composition of temporal and spatial count increments, ensuring that the realization is well-defined.
Any deviation from this fixed ratio would introduce path dependence in the assignment of separations, leading to frame-dependent inconsistencies and violating the requirement that M produce a unique and invariant realization in the System Frame. In this sense, the relation c = lf/tf replaces the assumption of a spacetime metric with a kinematic closure condition on admissible mappings within a count geometry. The formulation aligns with the requirement that any kinematic framework reproduce Lorentz-invariant structure in the appropriate limit [10,11], while avoiding the introduction of a continuous spacetime manifold as a primitive object.
1.2.2 The Internal Frame, System Frame, and Reference Frame
MQ defines physical relations through three distinct but interrelated constructs. The Internal Frame describes a discrete domain in which separations are defined strictly by integer counts nL and nT. The System Frame describes a continuous representation in which those counts are mapped to measurable quantities. And the Reference Frame describes the operational frame associated with measurement and comparison.
The Frames Principle states that all physical observables arise from the difference geometry between the Internal and System Frames, evaluated relative to a Reference Frame. This replaces the classical paradigm in which observables are defined solely relative to an observer or coordinate system.
Fig. 1. Count of lf describing the separation between two phenomenon in the System Frame, with discrete length evaluated in the Internal Frame. Modified from [9].
1.2.3 Right–Triangle Construction and Count Geometry
The geometric content of the Frames Principle is captured by the right–triangle representation in Fig. 1. Side a represents the reference count and is always assigned a count of 1. Side b represents the Internal Frame count and when that count is multiplied by lf it represents the distance associated with an interaction event. And the hypotenuse corresponds to the separation in the System Frame. This yields a count-based analog of the Pythagorean relation, where nL is the count defined in the Internal Frame and nL + QL encodes the discrete–continuous mapping difference. This construction is not merely illustrative. It defines the operational geometry from which all MQ expressions are derived. The orthogonality reflects the independence of the discrete count structure from its continuous representation, while their combination produces the measurable separation.
1.2.4 Emergence of the Discrete–Continuous Mapping
The mapping between the Internal and System Frame introduces a nontrivial geometric effect arising from the incompatibility between discrete count structure and continuous representation. This effect is encoded through the mapping component QL, which quantifies the deviation between count-defined separation in the Internal Frame and its realized measure in the System Frame. Because the discrete count structure cannot be represented exactly within a continuous domain, the mapping necessarily induces a correction to measured separation.
Unlike Lorentz contraction, which depends on relative velocity, this effect is purely kinematic and arises from the structure of the Frames mapping. Its magnitude depends on the count scale and vanishes in the large-count limit, ensuring consistency with classical continuum descriptions. In this sense, the mapping defines a scale-dependent deformation of measured distance that is intrinsic to the transition between frames.
This behavior is consistent with general constraints on discrete-to-continuum mappings in physical systems, where coarse-graining produces effective continuum behavior while retaining underlying discrete structure [12,13]. Within MQ, however, this effect is not an emergent statistical artifact but a deterministic consequence of the Frames Principle and therefore enters directly into the definition of measurable quantities.
A second consequence of the mapping arises from the evolution of count structure under the internal update index A. With each increment of the Internal Frame update index A, the effective relational region associated with an interaction undergoes a loss QL relative to the Internal Frame reference scale. Because this loss occurs below the reference count scale, it produces a cumulative displacement in the realized separation. At the level of the System Frame, this displacement manifests as curvature in the effective geometric description.
This kinematic origin of curvature can be expressed directly in terms of the mapping structure. In particular, the effective gravitational coupling associated with this displacement follows from the same count-based construction ([9], Appx. C):
where the factor 2QLnL represents the non-Lorentz length contraction term arising from the Frames mapping and θsi is a radial scalar describing the radial rate at which the universe expands. Notably, the contraction term is significant at interaction scales that are small – most prominently in electromagnetic interactions – and diminishes with increasing separation, recovering classical gravitational behavior in the macroscopic limit.
The appearance of this term at the kinematic level is central to the MQ framework. It establishes that curvature and coupling are not introduced independently but arise from the same underlying mapping structure that governs the relation between discrete counts and continuous measurement. As will be shown in later sections, this same structure is responsible for the unified emergence of electromagnetic and gravitational behavior from a single action through count-dependent realization under the Frames mapping.
1.2.5 Kinematic Sufficiency of the Triangle Construction
The right–triangle construction provides a complete kinematic description within MQ. The invariant ratio ensures consistency between temporal and spatial counts. The geometric relation defines measurable separation. And the frame mapping encodes all deviations between discrete and continuous representations. No additional geometric primitives – such as a metric tensor or connection – are required at this stage. Those structures, if they arise, do so only after coarse-graining and are not fundamental inputs to the framework.
This distinguishes MQ from both GR and gauge field theories. In GR, the metric is primary and defines geometry [2]. In gauge theories, fields are defined on a fixed background manifold [14]. In MQ, both geometry and interaction emerge from the same count-based construction.
1.3 Criteria for a Successful Unification
A theory that claims to unify distinct physical interactions must satisfy a set of well-established criteria that have emerged across more than a century of theoretical development. These criteria are not arbitrary. Rather, they reflect structural requirements that have been repeatedly identified in successful physical theories and in prior unification attempts. The purpose of this section is to state these criteria precisely, justify their necessity, and establish the standard against which the MQ framework will be evaluated in subsequent sections.
1.3.1 Single Underlying Kinematic Structure
A necessary condition for unification is the existence of a single underlying kinematic framework from which all interactions arise. Historically, successful theories such as electromagnetism and GR achieve internal coherence by grounding all observable phenomena in a common geometric or field-theoretic structure [1,2]. Conversely, the coexistence of multiple independent kinematic primitives – such as a spacetime metric for gravity and gauge fields for electromagnetism – signals an incomplete unification.
The requirement of a single kinematic structure ensures that all observables are derived from a common set of primitives. One, no interaction requires an independent geometric or algebraic substrate. Two, cross-domain predictions are meaningful without additional assumptions. In this way the criteria are both necessary and restrictive such that they exclude hybrid constructions in which distinct sectors are combined without eliminating their foundational independence.
1.3.2 Single Dynamical Principle
Beyond kinematics, a unified theory must possess a single dynamical principle, typically expressed through an action functional whose variation governs all interactions. The role of the action principle in modern physics is foundational. It provides a unified mechanism from which equations of motion, conservation laws, and symmetry relations are derived [15,16].
Formally, this requirement can be stated as:
There exists a single action functional S such that all physically admissible field configurations satisfy δS=0 under appropriate variations.
This condition ensures that: gravitational and electromagnetic dynamics are not introduced separately, conservation laws arise from symmetries of the same functional, and that no sector-specific equations are postulated independently. The absence of such a principle leads to theories that are descriptive rather than explanatory, lacking a unifying origin for their dynamical content.
1.3.3 Recovery of Established Physical Limits
A viable unification must reproduce established physical theories within their respective domains of validity. This includes, at minimum, the recovery of Maxwell’s equations in the appropriate weak-field or small-perturbation limit [1,5], the recovery of geodesic motion and curvature-based dynamics in the macroscopic gravitational limit [2], and compatibility with Lorentz invariance in contexts where Special Relativity (SR) is experimentally confirmed [10,11].
This requirement reflects a fundamental principle of the theoretical community: new theories must extend, not contradict, empirically validated results. In practice, this imposes strong constraints on any proposed framework, as it must reproduce distinct observed behaviors through a single underlying structure without introducing independent dynamical sectors.
1.3.4 Symmetry and Conservation Consistency
A unified theory must exhibit internal consistency through its symmetry structure. In modern physics, symmetries are not optional features but determine conservation laws through Noether’s theorem [15]. Accordingly, a unified framework must ensure that energy–momentum conservation arises from invariance under coordinate transformations, gauge invariance yields conserved currents and that all conservation laws emerge from the same underlying dynamical structure. These requirements are critical because they link mathematical consistency to physical observability. A theory that fails to produce the correct conservation laws from its symmetries cannot be considered complete.
1.3.5 Reduction of Independent Parameters
A defining feature of unification is the reduction of independent coupling constants and free parameters. In the Standard Model and GR, fundamental constants such as G, e, and ħ are introduced independently. A successful unification should instead demonstrate that such quantities arise from a smaller set of underlying parameters or from a single geometric or kinematic structure [6,7].
This criterion is essential for two reasons. First, it increases predictive power by reducing arbitrariness. And secondly, it indicates that seemingly distinct interactions share a common origin. Without parameter reduction, a theory may provide a formal unification but fail to achieve explanatory unification.
1.3.6 Predictive and Falsifiable Structure
Finally, a unified theory must produce new, testable predictions that distinguish it from existing frameworks. The requirement of falsifiability is central to the scientific method and ensures that unification is not merely a reinterpretation of known results. Such predictions may include deviations from classical behavior at specific count scales, new relationships between observables, or measurable corrections arising from count-dependent normalization within the unified structure. This criterion ensures that unification has empirical content and can be subjected to experimental validation.
1.3.7 Why These Criteria are Definitive
The criteria listed above are not independent. They form a tightly coupled set of requirements that collectively define unification. A theory that satisfies only a subset of these conditions cannot be considered fully unified for three reasons. One, a single kinematic structure without a single dynamical principle lacks predictive completeness. Two, a single action without parameter reduction retains unexplained arbitrariness. And three, recovery of limits without new predictions reduces to consistency rather than unification.
Historically, attempts at unification have failed precisely because they satisfy some but not all of these conditions. For example, higher-dimensional theories achieve geometric unification but do not eliminate independent parameters [3,4], while quantum gravity approaches may provide dynamical consistency without reproducing all classical limits [8]. Thus, these criteria are both inclusive – capturing all necessary aspects of unification – and exclude frameworks that do not fully resolve the structural separation between interactions.
1.4 Scope of the Present Paper
The present work is structured to evaluate whether the MQ framework satisfies the criteria for physical unification established in Sec. 1.3, while maintaining strict separation between foundational construction, empirical validation, and full field-theoretic reconstruction. The scope is therefore deliberately constrained. This paper establishes the kinematic and statistical basis for unification and demonstrates high-significance empirical concordance, while deferring the complete derivation of the emergent field equations and their tensorial structure to the appendices and subsequent work.
1.4.1 Primary Objective: Empirical Validation of the Frames Principle
The central objective of this paper is to test the Frames Principle through a statistically rigorous concordance analysis across physically independent implementations. The analysis evaluates whether a single count-based kinematic framework – defined by the Internal and System Frames, and their associated Frames mapping (Appx. I) – can simultaneously reproduce gravitational, electromagnetic, and cosmological observables without introducing independent sector-specific parameters.
This objective is operationalized through the construction of a comprehensive σ–concordance analysis, which compares MQ derived expressions to experimentally measured quantities across multiple domains. The methodology follows standard statistical practice to quantify agreement between prediction and measurement [43–46].
Within this framework, each implementation of the Frames Principle constitutes a physically independent test. Independence is defined not only by distinct observables but also by the absence of shared systematic dependencies, ensuring that aggregate significance reflects genuinely independent evidence rather than repeated sensitivity to the same underlying effects.
1.4.2 Role of the Concordance Analysis
Table I: Concordance Assessment of the Frames Principle Using Classical Expressions to Independently Compare 2010, 2014, 2018, and 2022 CODATA Datasets [19-22] | |||||
Implementations | 2022 | 2018 | 2014 | 2010 | w/o MQ |
MQ Tension Solutions (G, H0) | 6.63 | 6.63 | 6.63 | 6.61 | 0.00 |
MQ Tests of Length Contraction (𝐺, 𝛼) | 5.08 | 5.08 | 5.06 | 5.01 | 0.00 |
MQ Tests of Unification (G with μ0, a0, θsi) | 5.24 | 5.25 | 5.22 | 5.11 | 0.00 |
MQ Physical Constant Solutions (𝐺, 𝛼, 𝜃si, ħ, 𝜀₀, 𝜇₀, 𝑎₀) | 8.25 | 9.00 | 9.11 | 8.60 | 0.00 |
MQ Frames Principle (Includes all 11 implementations) | 8.74 | 11.9 | 9.39 | 8.48 | 0.00 |
The σ–concordance analysis presented in Table I serves as the empirical core of the paper. It is designed to address a central question: can a single kinematic framework, without adjustable coupling constants, reproduce experimentally measured quantities across distinct physical scales with statistically significant agreement? The table reports a global concordance analysis across independent degrees of freedom, using a right–tail p–value converted into an agreement sigma. The global assessments are grouped by discipline and span a broad range of count separations, allowing the empirical performance of the Frames Principle to be evaluated both by implementation class and across CODATA publications. From one publication to the next, the results show only modest variation, while the Frames Principle assessment remains at high significance.
Table I is therefore not auxiliary but foundational. It provides a direct test of parameter reduction (Sec. 1.3.5), a quantitative assessment of cross-domain consistency, and an empirical benchmark against which classical (Planck-based) formulations can be compared. Importantly, where expressions include the MQ-predicted length contraction, the “w/o MQ” column omits this term. This comparison isolates the contribution of the discrete contraction structure and distinguishes MQ expressions from the corresponding classical expressions obtained when the contraction term is removed. Because removal of this term reduces MQ’s fundamental measures to their Planck-form counterparts, the contrast provided in Table I tests whether the observed concordance is attributable specifically to the Frames mapping rather than to shared dimensional analysis or unit construction.
The summary provided in Table I is complemented by the detailed implementation-level concordance analysis presented in Appx. H. There, the full 2022 CODATA breakdown, methodological notes, and implementation-specific exclusions are presented. In this way, the main text establishes the empirical significance of unification at a glance, while Appx. H provides the full audit trail underlying that result.
1.4.3 Scope of Theoretical Development
While the MQ framework is capable of supporting further extensions, the present work already establishes a unified field-theoretic structure at the level required for physical unification. In particular, a single action defined on the count-based kinematic substrate is constructed and shown to generate both electromagnetic and gravitational behavior as distinct realizations of the same underlying dynamics. Electromagnetic behavior arises from evaluation of the action at the fixed interaction count defined by the electromagnetic demarcation, yielding an emergent Abelian gauge structure with associated Maxwell-type equations, while gravitational behavior corresponds to count-resolved realizations in which the mapping produces an effective metric description with geodesic dynamics and a mapping-dependent gravitational coupling.
In addition, the core symmetry and consistency relations are not deferred but demonstrated within the main development. Variation of the action with respect to the emergent geometric descriptor yields the stress–energy tensor, invariance under admissible diffeomorphic transformations yields covariant conservation, and invariance of the derivative-based action under gauge re-parameterization ensures the consistency of the energy–momentum tensor. These structures arise as co-emergent consequences of a single action defined through the Frames mapping between the Internal Frame and the System Frame, rather than being imposed independently. The result is a closed consistency chain linking gauge structure, gravitational response, and conservation laws within a unified kinematic origin.
The role of the appendices is therefore not to introduce these structures, but to provide their detailed formal development and explicit construction in equation form. The main text establishes their existence, interdependence, and physical necessity, while the appendices supply the extended derivations, normalization conditions, and structure-specific refinements required for full technical completeness.
This staging reflects a methodological choice, but not a limitation of scope. Unlike prior unification programs in which formal structure is introduced independently of empirical validation [6–8], the present work integrates both simultaneously. A unified action-based framework is constructed and shown to satisfy the required symmetry and consistency conditions, while its physical validity is established through high-significance concordance with observational data. This dual requirement ensures that the unification is not only mathematically coherent but empirically grounded, consistent with the principle that physical theories must ultimately be judged by their predictive and observational adequacy [16–18].
1.4.4 Delineation of What Is and Is Not Claimed
To maintain clarity while accurately reflecting the scope of the present work, the claims established in this paper are delineated as follows. First, a single count-based kinematic framework defined through the Frames Principle is shown to generate a unified dynamical structure from which both electromagnetic and gravitational phenomena emerge as distinct realizations of the same underlying action. Second, this framework yields explicit expressions for physical observables across multiple domains, and these expressions achieve statistically significant agreement with experimental data when evaluated through independent implementations of the Frames mapping. Third, the inclusion of the non-Lorentz length contraction term arising from the Internal Frame is shown to be necessary to achieve this level of empirical concordance.
In addition to empirical agreement, the paper establishes a coherent theoretical closure at the level required for physical unification. A single action functional defined on the count-based substrate is constructed and shown to generate, under distinct realizations determined by count separation, an emergent Abelian gauge structure with associated Maxwell-type equations when evaluated at the fixed interaction count defined by the electromagnetic demarcation, and an emergent geometric description with metric structure and geodesic dynamics for count-resolved realizations. The associated symmetry and consistency relations are likewise demonstrated. Variation of the action yields the stress–energy tensor, invariance under admissible transformations yields covariant conservation, and gauge invariance is preserved within the energy–momentum tensor. These structures arise as coupled consequences of the same kinematic origin rather than as independent postulates.
At the same time, several elements remain outside the scope of what is claimed here. We do not establish a fully general, closed-form tensorial reconstruction of all field equations across arbitrary scales, nor do we provide a complete treatment of quantum field-theoretic extensions, non-Abelian generalizations, or full renormalization structure. In addition, while the framework is shown to reproduce the relevant limiting behavior consistent with established electromagnetic and gravitational theories, a comprehensive comparison with all competing unification programs at the level of quantization and ultraviolet completion is not undertaken.
These limitations reflect scope control rather than structural incompleteness. The appendices provide detailed derivations of the action, symmetry relations, and mapping structure, while the main text establishes their interdependence and physical consequences. The result is a unified framework that is both empirically validated and theoretically coherent at the level necessary to support the central claim of kinematic unification, with further extensions reserved for subsequent development.
2. METHODS
2.1 Internal–System Mapping and Count Geometry
The Frames Principle asserts that all physically meaningful observables arise through a mapping from a discrete count-based configuration domain to a realized relational structure. In MQ, the Internal Frame is the discrete relational domain ω, whose primitive content consists solely of conserved count configurations and adjacency relations. Observable quantities do not exist intrinsically within ω. They arise only after realization through the Frames mapping, which induces the emergent System Frame reference structure ℛ. Geometry, continuity, and measurement are therefore not assumed a priori but emerge from the mapping itself.
This construction differs fundamentally from formulations that begin with a pre-existing spacetime manifold. The primary kinematic object is the count structure of the Internal Frame, while the continuum structures employed in physical measurement arise as realized encodings of that count structure. The role of the mapping is therefore not merely representational; it defines the conditions under which observables become physically meaningful.
2.1.1 Frames and Mapping Structure
Let ω'⊂ω denote a relational region of the Internal Frame. The Frames mapping is defined by
where ℛ is the System Frame reference structure and Ω is the realized System Frame image of the Internal Frame region ω'. A valid realization preserves the normalization, realization consistency, and holonomy constraints required by the Frames Principle. Consequently, physically observable quantities are associated with elements of Ω, not with elements of ω' directly.
Equation (2) establishes the fundamental distinction between Internal Frame and System Frame descriptions. The Internal Frame contains only discrete relational count structure, while the System Frame contains the realized relational encoding through which measurement is defined. Observable quantities therefore arise only after application of the Frames mapping and are represented by realized configurations in Ω, rather than by elements of the underlying count substrate itself.
The Frames mapping induces a realization measure on Ω. The corresponding System Frame encoded availability density is
where μM is the measure induced by the Frames mapping M on the realized configuration Ω, and dV is the associated System Frame volume element. The density ρS represents the realized encoded availability obtained from conserved Internal Frame count structure under the mapping and serves as the fundamental System Frame scalar from which normalized probabilities, expectation values, and continuum observables are constructed.
Equations (2) and (3) provide the minimal kinematic framework required for the remainder of the analysis. Equation (2) specifies how discrete count configurations acquire realized relational meaning through the Frames mapping, while Eq. (3) defines the corresponding System Frame encoded availability density induced by that realization. Together, these relations establish the discrete-to-continuous correspondence required by the Frames Principle and provide the foundation from which both fixed interaction scale realizations and curvature resolved realizations emerge within MQ.
2.1.2 Right–Triangle Construction and Count Geometry
The geometric consistency of the mapping is captured by a minimal relational construction. Consider a normalized reference count and an Internal Frame count nL. The mapped System Frame separation nL + QL is defined through a constraint relation that enforces consistency of count composition:
This relation is not a geometric axiom but a consequence of consistency between discrete count structure and its continuous embedding. It provides the minimal closure condition required for a valid Frames mapping.
2.1.3 Discrete–Continuous Mapping and Contraction Structure
The mapping M introduces a systematic deviation between Internal Frame counts and System Frame separations. This deviation is captured through a mapping dependent contraction term expressed at the level of count realization:
where nL is equal to the count of lf along side b and nL + QL describes side c, QL represents the non-whole count portion of the hypotenuse. It follows that
. This contraction is not Lorentzian. It does not arise from relative velocity but from the incompatibility between discrete count structure and continuous encoding. Unlike Lorentz contraction, which depends on kinematic state, MQ contraction depends on the radial scaler rate θsi of the expanding frame of the universe, DU = 2θsiAU ([9], Appx. AZ). Consequently, all System Frame observables inherit a scale dependence through θsi = lfmf/2tf, affecting inferred distances, coupling strengths, and geometric relations.
2.1.4 Kinematic Role of the Mapping
The Frames mapping simultaneously performs three roles. It embeds discrete count structure into a continuous representation. It introduces count-dependent length contraction via 2QLnL ([9], Appx. D). And it provides a unified origin for geometric and interaction structure, including the emergence of curvature as the cumulative realization of mapping-induced deformation over extended count separation. In this framework, structures typically introduced independently – such as metrics, curvature, or gauge fields – emerge from the properties of M, consistent with the derivation of gauge structure from underlying symmetries.
2.1.5 Relation to Classical Limits
In the large-count limit,
and the mapping reduces to a classical continuous description. In this limit discrete corrections vanish, the System Frame geometry becomes effectively smooth and standard relativistic and field-theoretic behavior is recovered. This is consistent with renormalization and continuum limit arguments in field theory.
2.1.6 Section Boundary
The contraction structure introduced here defines the kinematic origin of geometric scaling and interaction strength. Its formal realization in terms of curvature, metric normalization, and coupling emergence requires a tensorial treatment. These results are developed in Appx. D, where discrete–continuous mapping is extended to curvature scaling and gravitational coupling.
2.2 Fundamental Measures and the Role of θ
MQ is defined on a discrete substrate within the Internal Frame, where all physical quantities arise from integer-valued counts of the fundamental measures lf , mf and tf. These measures constitute the primitive elements of the count structure and are defined on the configuration domain ω, with relational subsets ω'⊂ω supporting finite count measures NI(ω',A). No geometric or continuum structure is assumed at this level. Instead, all continuum descriptions arise through the Frames mapping M:ω→ℛ, which induces the System Frame representation. The only non-trivial invariant parameter admitted by this structure is the dimensionless scalar
which encodes the relative scaling of the fundamental measures. This parameter is invariant under admissible transformations of the Internal Frame count assignments and therefore uniquely governs the mapping between discrete and non-discrete descriptions through the normalization constraints imposed by the Frames mapping.
Within this framework, all emergent physical scales are determined by how count densities and adjacency fluxes transform under M. In particular, the characteristic count length associated with electromagnetic interactions is fixed by the electromagnetic demarcation at nL = 84.60055 ([9], Appx. AB, AE, AM). The count of lf defines a distinguished scale in the Internal Frame at which boundary flux relations yield stable, repeatable interaction outcomes in the System Frame. This scale arises from the normalization constraints imposed by the Frames Principle and the requirement of consistent realization under repeated measurement mappings. While a calculation of this value yields slightly different results following the 5th digit after the decimal, analysis shows that the value is determined geometrically by ([9], Appx. AC)
The parameter θsi ([9], Appx. AD) is an intrinsic constant of the MQ count structure, but its numerical value is fixed through empirical input, most directly via the fine structure constant. While it may also be expressed in terms of the fundamental measures, such representations are not independent, as they require additional experimentally determined quantities (e.g., the electron mass and Bohr radius) and therefore do not constitute a first principles derivation. Its physical significance emerges only after the Frames mapping induces a non-discrete relational encoding, at which point effective dimensional quantities and interaction strengths appear as functions of θsi. No reduction arguments are introduced at this stage. These follow from the mapping-dependent contraction structure and its extension to curvature and coupling, developed in Appx. D and the subsequent derivation of interaction structure in Sec. 3.
2.3 Why Gravity and Electromagnetism Are Expected to Share One Substrate
The preceding sections have established three essential elements of the MQ framework: the Frames Principle as the defining structure of measurement, the existence of an Internal Frame governed by discrete count relations, and a nontrivial Frames mapping that generates the observable System Frame. The question addressed in this section is whether these structures admit multiple independent dynamical substrates – one for gravitation and one for electromagnetism – or whether they necessarily imply a single underlying kinematic origin. Within MQ, the latter is not an assumption but a consequence of the construction.
2.3.1 Uniqueness of the Underlying Kinematic Substrate
The Internal Frame is defined as a configuration domain ω supporting admissible count assignments and a Frames mapping M:ω→ℛ into the System Frame structure ℛ. Valid realizations of the mapping exist on referenceable domains U⊂ω satisfying normalization, unique realization, and holonomy-free closure. By construction, physical observables arise exclusively through the realized image M(U). There is no independent geometric or dynamical structure in the System Frame beyond what is induced by M.
It follows that all interactions accessible to observation must be expressible as distinct realizations of the same mapping applied to the same underlying count structure. Introducing separate substrates for different interactions would require either multiple independent configuration domains ω, or multiple incompatible mappings acting on a shared domain.
The first possibility violates the requirement of a single referenceable universe domain U, which must satisfy normalization, unique realization, and holonomy-free closure across all admissible interactions. The second possibility introduces inconsistencies in the reference structure ℛ, since distinct mappings would in general fail to preserve common invariants on shared reference cycles γ, leading to observable contradictions.
Therefore, the Frames Principle enforces a single admissible mapping structure, and hence a single kinematic substrate, from which all interactions must emerge.
2.3.2 Electromagnetism and Gravitation as Distinct Mapping Realizations
Given a single substrate, the observed distinction between electromagnetic and gravitational phenomena arises from different interaction distances realized within the same Frames mapping, rather than from fundamentally different underlying structures. This perspective is consistent with established features of both interactions. Electromagnetism is characterized by gauge structure and local field variations, as formalized in Maxwell theory and its quantum extensions [1,5,17]. Gravitation is described by geometric relations associated with spacetime curvature and geodesic motion [2,18].
In MQ, these differences are reinterpreted as consequences of how the Frames mapping resolves discrete count structure at different interaction distances. For all known electromagnetic interactions—specifically blackbody radiation, charge couplings, and elementary charge—the interaction occurs at a fixed count separation given by the electromagnetic demarcation, nL = 84.60055, the count of lf at which electromagnetic interactions are realized. By contrast, gravitational interactions are evaluated at the actual interaction distance. The difference relevant to the non-Lorentz length contraction is therefore not that gravitation constitutes a fundamentally separate effect, but that the interaction distance entering the mapping differs.
The non-Lorentz contraction effect predicted by MQ is most significant at interaction distances below a few hundred counts of lf and diminishes rapidly with increasing distance. Electromagnetic interactions probe a fixed finite-count distance at which this effect remains non-negligible, whereas gravitational interactions are typically realized at larger distances for which it is negligible. The distinction therefore arises from count separation within the same mapping structure, not from separate underlying substrates.
These descriptions are not independent sectors but complementary realizations of the same underlying count geometry. The distinction follows from interaction distance, normalization, and the relative magnitude of the Informativity differential within the Frames mapping.
2.3.3 Parameter Reduction as Evidence of a Shared Substrate
A central empirical indication that gravity and electromagnetism share a common origin is the reduction of independent constants achieved within MQ. As demonstrated in prior work, quantities traditionally treated as independent – such as the gravitational constant G, the fine structure constant α, and Planck-scale quantities – can be expressed in terms of shared fundamental measures and mapping relations [9,19]. This contrasts with conventional formulations, where electromagnetic and gravitational couplings are introduced independently and lack a unifying derivation [16,17]. The MQ framework instead yields interdependent expressions, indicating that both interactions arise from the same structural parameters.
The concordance results summarized in Table I support this conclusion. Independent measurements across gravitational and electromagnetic domains are simultaneously reproduced within a single parameter framework, without introducing interaction specific adjustments. This level of cross-domain agreement would be statistically improbable if the underlying substrates were distinct.
2.3.4 Empirical Cross-Consistency: The Hubble Tension
The resolution of the Hubble tension provides a concrete example of how a single substrate manifests differently across interaction channels. Electromagnetic distance ladder measurements and gravitational inferences yield systematically different expansion rates. In MQ, this discrepancy is not attributed to new physics in either description but to the fact that each probes a different realization of the Frames mapping.
Specifically, electromagnetic observations correspond to a mapping more directly tied to the Internal Frame count structure, while gravitational inferences reflect a mapping dominated by System Frame normalization at effectively macroscopic interaction distances. The resulting difference in MQ inferred distances yields a 3.35 sigma concordance, quantitatively consistent with the SPT-3G [20] and PANTHEON+ [21] measurements. A deeper explanation is provided in Ref. [22]. Importantly, this explanation is only coherent if both measurement channels originate from the same underlying substrate. If electromagnetism and gravitation were fundamentally independent, there would be no reason to expect a systematic, quantitatively predictable relation between their respective measurements.
2.3.5 Structural Constraint from Conservation and Invariance
The requirement of a shared substrate is further reinforced by conservation and invariance principles. In classical and quantum field theory, conservation laws arise from symmetries via Noether’s theorem [15]. In MQ, these symmetries are not imposed externally but emerge from the structural constraints of the Frames mapping, including normalization and holonomy-free closure.
Because these constraints apply globally to the mapping M, they must hold across all interaction realizations. Separate substrates would generically lead to incompatible symmetry structures, violating conservation laws when interactions are combined. The observed consistency of conservation principles across electromagnetic and gravitational phenomena therefore supports a unified origin.
2.3.6 Classical Limit and Consistency with Established Theories
In the appropriate limits, the MQ framework recovers the standard descriptions of both electromagnetism and gravitation. When the mapping-induced contraction becomes negligible, the System Frame representation approaches a continuous description in which Maxwell-type equations govern electromagnetic behavior and Einstein’s field equations govern gravitational dynamics. This ensures consistency with the well-tested predictions of both theories [1,2,16,18], while identifying their origin in a common kinematic structure.
The distinction between interaction channels arises through how the Informativity differential enters under the Frames mapping. Electromagnetic interactions are realized at a fixed interaction count defined by the electromagnetic demarcation nL = 276/θsi, for which the mapping-induced contraction is constant. This yields a stable normalization of the System Frame realization and supports the emergence of a local Maxwell-type description.
Gravitational interactions, by contrast, are realized at count separations corresponding to the physical distance between interacting bodies. The Informativity differential therefore varies with separation 2QLnL → 1, introducing a scale-dependent normalization while preserving the geometric structure of the field equations. The resulting dynamics are described by Einstein’s equations in the large-count limit.
3. RESULTS
3.0 Single Action Principle
The preceding sections established that all observable structure arises from a single Frames mapping M:ω→ℛ acting on a unified Internal Frame configuration domain (Appx. I). Equally important, Section 1.4.2 demonstrated that this mapping is not merely a formal construct, but one that satisfies a stringent empirical constraint: a global σ–concordance across eleven physically independent implementations spanning gravitational, electromagnetic, and cosmological scales (Table I; Appx. H). Any proposed dynamical formulation must therefore reproduce this cross-domain agreement without introducing independent sector-specific couplings.
The logical consequence of these combined structural and empirical results is that the dynamical description of physical systems must itself be unified. There must exist a single scalar functional whose stationary realizations generate all admissible System Frame observables and preserve the concordance structure already established. This object is referred to as the MQ action (Appx. J).
In contrast to conventional formulations – where distinct actions are postulated for gravitational and electromagnetic formulations – the MQ framework requires that all dynamics emerge from a single kinematic origin. This requirement aligns with the role of action principles in classical and quantum field theory, where stationary action selects physically realizable trajectories and field configurations [16,17]. However, in MQ the action is not defined on a pre-existing manifold. Rather, it is induced by the admissibility constraints of the Frames mapping itself. In this sense, the action is not an independent postulate, but the unique dynamical object consistent with both the closure structure of the mapping and the empirically observed concordance across physical domains.
3.1 The MQ Action as the Common Dynamical Object
We define the MQ action as a scalar functional over admissible System Frame encodings induced by the Frames mapping:
with the associated Lagrangian density written as
Here ρR is the System Frame encoded availability density defined on the realized configuration Ω=M(ω')⊂ℛ, ∇ρR captures variation within the encoded continuum representation, lf, mf, and tf are the MQ fundamental measures, and dμ is the induced measure on Ω. This notation is consistent with the current term definitions (Appx. A), in which ℛ denotes the relational codomain of the Frames mapping and physically realized configurations correspond to subsets Ω⊂ℛ.
The triplet of fundamental measures defines the primitive dimensional structure of the MQ framework. These measures are not independent in their physical role. They are linked by the invariant scalar combination θsi = lfmf/2tf, which constitutes the unique dimensionless parameter governing the relative scaling between the Internal Frame and the System Frame.
While θsi does not appear explicitly in Eq. (9), it organizes the admissible structure of the Lagrangian density ℒMQ by constraining how the fundamental measures enter all dimensionless combinations. In this sense, θsi functions as the structural invariant of the theory, whereas lf, mf, and tf provide its dimensional realization. The MQ action is therefore specified at three distinct but connected levels.
At the primitive level, the dynamical structure is fixed by the admissible dependence of ℒMQ on the encoded availability variables and the fundamental measures, prior to any identification with empirical units. At the invariant level, all physically relevant dimensionless combinations are functions of θsi. In particular, the electromagnetic demarcation and relative frame scalings depend only on θsi (Appx. J), for example nL = 276/ θsi, which fixes the electromagnetic interaction scale in units of lf. At the calibrated level, a physical realization of the theory is obtained by identifying the MQ measures against experimentally defined quantities already used elsewhere in the paper, so that numerical values for lf, mf, tf and θsi are fixed and conventional physical constants appear as composite quantities. This calibration and its parameter-reduction consequences are developed later in the parameter-reduction discussion of Sec. 3.5.5.
Crucially, no independent coupling constants are introduced at the level of the action. All such constants arise only after calibration as derived quantities from the fundamental measures and their invariant relation. The Lagrangian therefore encodes the dynamical content of the theory at the primitive level, while higher-level physical laws emerge through invariant structure and calibrated realization.
The admissible form of ℒMQ is constrained by the requirements of normalization of encoded availability, holonomy-free closure on contractible reference cycles γ, and invariance under frames automorphisms Φ. These constraints restrict admissible terms in the Lagrangian density, analogously to the way symmetry principles constrain Lagrangians in gauge theory [5,15].
A key structural feature is that the action depends only on quantities derived from the Frames mapping. No independent geometric metric or external gauge field is introduced at this stage. Metric and gauge structures arise only as emergent descriptions in appropriate limits. In this respect, the MQ action plays a formal role analogous to geometric actions in GR, while differing fundamentally in that curvature is not assumed a priori. Rather, geometric structure is treated as a derived consequence of the mapping between discrete count structure and continuum encoding.
3.1.1 Variational Principle and Admissible Field Variations
Physical realizations correspond to stationary points of the MQ action under admissible variations of the encoded availability density, δSMQ=0. However, not all variations δρR are permitted. Admissible variations must preserve the defining constraints of the Frames mapping:
Normalization constraint: total encoded availability is conserved under variation,
Holonomy constraint: variations must not introduce nontrivial holonomy on contractible cycles,
Realization constraint: variations must preserve unique realization mappings, ensuring that outcome-to-record correspondence remains injective.
In addition, admissible variations must preserve the induced boundary–adjacency structure inherited from the Internal Frame, ensuring that flux relations across ∂Ω remain consistent with the underlying count continuity relations, and that the encoded availability density remains a valid non-negative measure on Ω.
Under these constraints, the Euler–Lagrange equation associated with Eq. (9) takes the form:
This equation defines the fundamental dynamical condition for the encoded availability field. Its structure mirrors standard variational formulations in field theory [16,17], but its interpretation is distinct. It governs admissible encodings of discrete count structure rather than the evolution of fields on a pre-existing spacetime manifold and is restricted to variations consistent with the Internal Frame continuity and boundary flux structure induced by the Frames mapping.
3.1.1.1 Emergent Temporal Structure from Internal Frame Ordering
In MQ, temporal structure is not introduced as a primitive coordinate but emerges from the ordered progression of Internal Frame configurations indexed by A. The mapping from Internal Frame configurations to System Frame observables is given by the Frames mapping M:ω→ℛ, with realized configurations Ω(A)=M(ω'(A))⊂ℛ, where ω'(A)⊂ω denotes the relational region at update index A. Temporal structure in the System Frame is therefore induced not by mapping alone, but by the ordered sequence of mapped configurations.
Temporal evolution in the System Frame therefore reflects a realized ordering of count configurations under M, rather than an independently defined continuous parameter. This construction is consistent with the Frames Principle, which requires that all observable quantities arise from relational structure rather than assumed background coordinates [15]. Consequently, temporal observables must be defined through measurable frame-dependent quantities.
Within this structure, temporal expansion is characterized through frame-resolved expansion rates. The System Frame expansion rate Hsys is the System Frame realization of the expansion parameter, while the Internal Frame expansion rate Hint is the Internal Frame realization associated with the ordering of count configurations over A. These quantities differ because the System Frame encodes interaction-constrained realizations – most notably through the electromagnetic demarcation – whereas the Internal Frame describes the full count evolution without observational constraint.
When accounting for these differences we find that Hsys = π/θsiAU and Hint = (2θsi-π)/θsiAU ([22], Eqs. 84-85). The emergent cosmological term is therefore expressed in a frame-resolved manner as
These relations follow from the MQ formulation of cosmological expansion and preserve its standard dependence on the Hubble parameter in relativistic cosmology [16,23,24]. In MQ, however, the distinction between Hsys and Hint reflects the discrete–continuous structure induced by the Frames mapping, rather than observational uncertainty or model-dependent corrections.
A complete derivation of Hsys and Hint, including their reduction to MQ fundamental measures and their role in resolving discrepancies in cosmological observations, is provided in [22]. The present formulation emphasizes that temporal structure in MQ emerges from a frame-dependent realization of count evolution and is not defined through direct differential correspondence between A and an externally imposed time coordinate.
3.1.1.2 Consistency with the Variational Structure
Under this identification, differential operators appearing in the MQ action are not primitive structures but arise as System Frame representations of normalized variation in the underlying Internal Frame count configuration. In the Internal Frame, all variation is defined discretely through adjacency relations and count redistribution governed by the conservation structure. The Frames mapping, together with the normalization functional, induces a continuum encoding in which these discrete variations are represented by differential operators acting on System Frame fields such as the encoded availability density.
The Euler–Lagrange equation therefore simultaneously enforces Internal Frame admissibility—through variation of the action with respect to realizable count configurations – and System Frame dynamics – through the induced differential structure acting on the continuum-encoded fields. No independent temporal degree of freedom is introduced. Apparent time derivatives arise from the mapping of the Internal Frame update index into the System Frame representation and reflect the normalization of sequential count redistribution rather than an underlying spacetime primitive.
3.1.1.3 Conservation Laws
Conservation laws arise directly from invariance of the MQ action under admissible transformations. This is consistent with Noether’s theorem, which relates symmetries of the action to conserved quantities [15]. In MQ, these symmetries correspond to invariances of the Frames mapping itself, rather than to transformations of an external spacetime.
3.1.2 Scale Dependence and Emergent Realization under the Frames Mapping
The MQ action admits scale-dependent realizations determined by the relative contribution of derivative structure and mapping-induced deformation within the Frames mapping. Both non-Lorentz contraction and emergent curvature arise from this same mapping-induced deformation, with curvature representing the geometric manifestation of the relation between the Internal and System Frame. These behaviors arise as scale-dependent realizations of a single kinematic construction governed by the invariant scalar.
The non-Lorentz contraction associated with the discrete structure of the Internal Frame is formalized as the Informativity differential. This quantity characterizes the deviation between relational separation in the Internal Frame and its encoded representation in the System Frame, given by 2QLnL. It applies strictly to realized spatial separation, reflecting a mapping-induced effect in the three-dimensional relational structure of the System Frame. The Informativity differential is greatest at small count separations and decreases rapidly with increasing separation, becoming negligible beyond a few hundred counts of lf. Mass and time, being singular in dimension, do not admit this form of mapping-induced contraction or curvature.
Notably, electromagnetic interactions are uniquely realized at a fixed count separation given by the electromagnetic demarcation. In contrast, interactions not fixed at the electromagnetic demarcation are realized across continuous count separations, including at small scales, where mapping-induced deformation remains locally significant. At larger count separations, such as those relevant to gravitational interactions, the Informativity differential becomes negligible, and the mapping approaches a smooth relational encoding. These realizations arise from the same action without the introduction of independent structures or coupling parameters. The distinction between electromagnetic behavior and gravitational curvature is therefore determined solely by how the Informativity differential enters through normalization at the electromagnetic demarcation versus its negligible contribution in count-resolved realizations across the physical domain.
3.1.3 Electromagnetic Limit
The electromagnetic demarcation corresponds to a fixed interaction count distance, which is resolved through three independent constructions. They are given by charge couplings, blackbody radiation, and elementary charge ([9], Appx. AB, AE, AO), respectively:
Each expression independently resolves the same interaction scale to seven digits. As such, we commonly use the first expression which offers the greatest precision, nL = 84.60054567(93). Importantly, the correlated results indicate that the electromagnetic demarcation is not a free parameter but a constrained geometric property of the Frames mapping.
The origin of this expression is clarified through the discrete structure of quantization ratios ([9], Appx. AC). The admissible solutions are restricted by the requirement that products of count and the invariant scalar yield integer-resolved values in the Internal Frame. In particular, only one combination satisfies this condition within the relevant range: nLθsi = 276 such that rq = nLθsi/⌈ nLθsi⌋.
This constraint uniquely identifies the electromagnetic interaction scale. Neighboring integer combinations (Table II) do not satisfy the required integer closure under quantization ratios and therefore do not correspond to admissible realizations. Within the corresponding count range, only a finite number of integer-resolved configurations exist, and only the value associated with nθ = 42 yields a solution consistent with the observed electromagnetic scale. This establishes the relation between the internal count nθ = 42 and the measured interaction distance 84.60055lf, where the latter represents the System Frame encoding of the former under the Frames mapping.
Table II. Quantization ratios rq for nL with respect to the Internal Frame.
Corresponding Count nL | Parameters | ||
rq | nLθsi | nθ | |
82.7614033 | 0.99819405 | 270 | 41 |
83.0679271 | 1.00014885 | 271 | 42 |
83.3744508 | 1.00014885 | 272 | 42 |
83.6809745 | 1.00014885 | 273 | 42 |
83.9874982 | 1.00014885 | 274 | 42 |
84.2940220 | 1.00014885 | 275 | 42 |
84.6005457 | 1.00014885 | 276 | 42 |
84.9070694 | 1.00014885 | 277 | 42 |
85.2135931 | 1.00201988 | 278 | 43 |
The dynamics reduce to conservation of the discrete measurement availability count nI(ξ,A) within the Internal Frame, expressed as
Here JI denotes the Internal Frame adjacency count-flux object whose net contribution at relational cell ξ is evaluated by (divadjJI)(ξ,A). The relation expresses local conservation of measurement availability entirely within the discrete relational adjacency structure of the Internal Frame. The adjacency divergence operator measures the net count imbalance associated with a relational cell through admissible adjacency transfers and provides the local conservation structure governing redistribution of count across the relational domain.
Only after application of the Frames mapping does this conserved count structure admit realization within the System Frame. Under mapping normalization, the conserved count, adjacency flux, and associated count imbalance are realized as continuum quantities defined on the emergent relational structure. The resulting continuum conservation relations therefore do not constitute independent postulates but arise from the realization of conserved Internal Frame count under the Frames mapping.
Within MQ, electromagnetic and gravitational behavior originate from the same conserved count substrate governed by the MQ Action and constrained by the MQ variational principle. Electromagnetic behavior corresponds to realization at the fixed interaction scale defined by the electromagnetic demarcation, where the Informativity differential remains significant and fixed by count separation. Gravitational behavior corresponds to realization in the curvature-resolved regime, where the same mapping-induced structure is evaluated across varying count separations. Both descriptions therefore emerge from a common conservation framework and represent distinct realizations of the same underlying count structure under the Frames mapping.
3.2 Fixed Interaction Distance and Emergent Abelian Structure
At the electromagnetic demarcation, the MQ action for electromagnetic interactions reduces to a local form evaluated at a single count separation, such that the mapping-induced normalization – and therefore the Informativity differential – remains constant across the interaction domain. This behavior is specific to the electromagnetic demarcation and contrasts with the count-resolved realization of the gravitational case. In this limit, the Lagrangian density introduced in Eq. (9) simplifies to the effective local form
where 𝒦 is not an independent coupling parameter, but an effective normalization coefficient fixed by the underlying fundamental measures (lf, mf, tf) and the electromagnetic interaction distance. Equation (18) therefore represents the reduction of the MQ action.
Applying the Euler–Lagrange equation to Eq. (18) gives ∇⋅(𝒦∇ρR)=0. For fixed 𝒦, as applies to the electromagnetic demarcation, this reduces to
up to normalization-preserving constraints. To connect with standard field representations, we define the System Frame log gradient availability field
This field encodes fractional variation in encoded availability density and provides the natural local connection associated with this fixed distance realization. Since 𝒜 is defined as the gradient of a scalar, the commutator of successive System Frame derivatives vanishes,
which is the local structural condition underlying Abelian behavior in this context.
The resulting field equations therefore exhibit linearity and locality. Within MQ, these properties arise because the Informativity differential is fixed by the interaction count at which electromagnetic interactions are realized, so the mapping-induced normalization enters only as a constant and does not contribute to variation across the interaction domain. No independent gauge structure is introduced. Instead, gauge-like behavior emerges from the invariance of the Frames mapping under admissible transformations. This establishes the electromagnetic realization as a fixed interaction-count limit of the MQ action.
3.2.1 Gauge Transformation and Commutativity
The encoded availability density ρR admits a multiplicative scaling freedom consistent with the System Frame realization of the Internal Frame count structure. Consider the transformation
where χ is a smooth scalar function on the System Frame domain ℛ. Under this transformation, the logarithmic gradient field that enters the MQ action transforms as
where A≡∇lnρR is defined by the derivative structure of the encoded availability density. The transformation law follows directly from the identity
and therefore, arises from the multiplicative scaling freedom of ρR. Because the transformation parameter χ enters additively and independently of A, successive transformations satisfy
Thus, the transformation group is Abelian.
This establishes that the emergent gauge structure is U(1), consistent with classical electromagnetism [1,17]. Crucially, this structure is not imposed axiomatically but follows from the intrinsic scaling of the encoded availability density under the Frames mapping. Therein, the Frames mapping demonstrates that gauge symmetry arises as a kinematic consequence of the construction.
3.2.2 Noether Current and Maxwell-Type Equations
The invariance of the derivative-only MQ action under the transformation (Eq. 22) implies the existence of a conserved current via Noether’s theorem [15]. The associated current is obtained by considering infinitesimal variations χ→ϵχ, yielding
where δρR=χ ρR follows from Eq. (22), and ℒρ denotes the derivative-only Lagrangian density expressed in terms of ρR and its derivatives. Using the log gradient structure 𝒜≡∇lnρR, and the derivative dependence of ℒρ, one obtains
which is fully determined by the encoded availability density and its induced gradient field. This current satisfies the continuity equation
consistent with conservation arising from the underlying Internal Frame count structure under the Frames mapping.
To establish correspondence with electromagnetic field theory, define the field strength tensor
with 𝒜μ≡(ϕ,𝒜) constructed from the log gradient field. The resulting field equations take the form
which are the Maxwell-type equations governing an Abelian gauge field [1,25].
Thus, within MQ, Maxwell’s equations emerge as the Euler–Lagrange and Noether consequences of the derivative-only bound of the single MQ action.
3.2.3 Interpretation of the Electromagnetic Demarcation
The realization of electromagnetic interactions corresponds to a well-defined condition on the discrete count structure determined by the Frames mapping. Within MQ, electromagnetic interactions occur at a fixed Internal Frame count scale
which defines the electromagnetic demarcation. This scale follows from the invariant scalar structure governing the mapping between the Internal and System Frame, as established in Sec. 2.3.
At this count scale, the contraction term 2QLnL is fixed. As a result, it contributes as a constant normalization to the MQ action and does not enter into local variation of the encoded availability density. The Euler–Lagrange structure therefore reduces to a form governed entirely by local variation, with the contraction structure implicitly encoded through normalization.
This produces an effective field description characterized by commutative structure and linear superposition, consistent with the emergence of an Abelian gauge structure. The resulting equations are therefore of Maxwell type in the appropriate limit, in agreement with the established role of gauge symmetry in electromagnetic phenomena [1,5,17].
3.3 Gravitational Limit
The gravitational limit of the MQ framework arises at large Internal Frame count separations nL. In this limit, the non-Lorentz contraction term 2QLnL approaches its asymptotic value and ceases to contribute to variation in the Frames mapping. This behavior follows directly from the discrete–continuous mapping structure, such that contraction effects decay rapidly with increasing count scale. As a result, gravitational interactions are realized at count separations where the mapping can be effectively evaluated near its upper bound. We often omit the term from leading-order expressions without loss of accuracy. The dynamics are then governed by global constraints imposed on the encoded availability density ρR through normalization and holonomy-free closure of the Frames mapping.
Variations in ρR across extended domains produce curvature-like effects that are naturally interpreted as a metric structure. This interpretation is consistent with the geometric description of gravitation in GR, where curvature arises from global consistency conditions on spacetime [2,18]. To formalize this emergence, the coarse-grained mapping admits an effective metric tensor
defined implicitly through the normalization and relational consistency conditions of the encoded density field. The resulting dynamics are governed by geodesic propagation in this emergent geometry, further developed in Appx. E.
Importantly, this does not represent a distinct dynamical sector. Both electromagnetic and gravitational behavior arise from the same MQ action functional, with the contraction magnitude determined solely by count separation. At the fixed interaction count associated with the electromagnetic demarcation, the Informativity differential is also fixed. At larger separations, its magnitude becomes negligible. The distinction between field-theoretic and geometric descriptions therefore reflects how the Frames mapping is evaluated across count separation as opposed to the introduction of separate physical mechanisms.
3.3.1 Coarse-Graining of Count Geometry
Coarse-graining of count geometry is defined through the realization of conserved Internal Frame count structure under the Frames mapping M:ω→ℛ, which maps relational count configurations defined on the configuration domain ω into the realized System Frame relational structure ℛ. Here, ω'⊂ω denotes a bounded relational region composed of adjacency-linked relational cells ξ, with realized configuration Ω=M(ω')⊂ℛ.
In the fine-grained description, the primitive quantity is the discrete measurement availability count nI(ξ,A), defined on the relational adjacency structure of the Internal Frame. Redistribution of count between neighboring relational cells is described by the adjacency count-flux object JI, and local conservation of measurement availability is governed by the Internal Frame continuity relation
Here JI denotes the Internal Frame adjacency count-flux object, while (divadjJI)(ξ,A) measures the net count imbalance associated with relational cell ξ arising from admissible adjacency transfers. No geometric, coordinate, vector, or continuum structure is assumed. Equation (32) expresses conservation entirely within the discrete relational structure of the Internal Frame.
For relational regions ω'⊂ω sufficiently large compared with the fundamental length scale lf, a coarse-grained description becomes admissible. The local Internal Frame count density is defined by adjacency averaging of the primitive count field,
where Adj(ξ) denotes the set of admissible neighboring relational cells associated with ξ, and ∣Adj(ξ)∣ is its cardinality.
The total conserved count associated with a relational region is
which defines the regional measurement availability contained within ω'.
Summing Eq. (32) over the relational region yields the regional conservation relation
where the boundary count-flux is
The quantity ϕI(∂ω',A) represents the net outward transport of measurement availability across the adjacency boundary ∂ω'. It is an exact discrete count-flux and does not correspond to a geometric surface integral.
The coarse-grained density ρI therefore introduces no new physical structure. It provides a locally averaged representation of conserved Internal Frame count while preserving the underlying conservation relations. Through the Frames mapping, the conserved count structure encoded by nI, NI, JI, and ϕI admits a mapping normalized realization within the System Frame, where continuum observables are defined. The resulting continuum description is therefore not an independent postulate but a realization of conserved count under the Frames mapping, consistent with the Frames Principle
Nontrivial structure emerges when the Frames mapping cannot be globally trivialized across extended relational regions. In such cases, aggregation of local mappings introduces residual incompatibility in the closure of reference information around relational cycles. Let γ⊂ω be a closed reference cycle. The corresponding holonomy functional is ℋ(γ). A mapping defect is present whenever ∃ γ⊂ω' such that ℋ(γ)≠0.
More generally, the defect class associated with the relational region is
Equation (37) identifies the simultaneous presence of persistent boundary count-flux and nontrivial holonomy as the condition for a genuine mapping obstruction. The defect is therefore not merely a local imbalance in adjacency transfers but a global obstruction to extension of a holonomy-free Frames mapping across the relational domain.
Under coarse-graining, these discrete defects are encoded in the spatial variation of ρR, providing the precursor to emergent geometric structure in the System Frame. At this stage, however, no metric or curvature object has yet been introduced. The result is solely a nontrivial organization of encoded availability across the relational domain induced by the conservation, flux, and closure properties of the underlying Internal Frame count structure.
Thus, coarse-graining serves as the mechanism by which discrete count structure becomes compatible with continuum representation while preserving the essential mapping constraints that give rise to emergent geometric behavior in subsequent sections.
3.3.2 Emergent Metric Structure
The emergence of a metric structure follows from the requirement that the System Frame encoding support consistent comparison of encoded availability across neighboring relational regions. Following Sec. 3.1, the coarse-grained encoded availability density ρS defines the primary scalar field on the realized relational domain. From this, we construct the System Frame log gradient field
which is well-defined under the continuum encoding induced by the Frames mapping. This object arises from the mapped representation of Internal Frame count structure and has no counterpart in the Internal Frame. In regions where the Frames mapping is locally trivializable, the field 𝒜μ is integrable, and its circulation over any contractible loop vanishes,
This corresponds to a regime in which the coarse-grained structure admits a flat representation, consistent with the absence of mapping defects. However, when the mapping fails to be globally trivializable, the circulation becomes nonzero over closed relational cycles,
indicating the presence of residual mismatch inherited from the discrete adjacency structure. This non-integrability defines a connection structure in the System Frame.
The associated antisymmetric field strength is
which encodes the local failure of integrability of the log gradient field. This object arises directly from the mapping of Internal Frame defects and is therefore a derived quantity.
To construct a metric structure, we consider second-order variations in realized separation. The natural quadratic form governing local variations is defined on a local coordinate chart xμ of the emergent System Frame as
where the metric tensor
characterizes the local realization of count resolved separation under the Frames mapping.
The continuum description admits a direct count based realization. In MQ (see Fig. 1), the fundamental realized separation is determined by
where nL is the Internal Frame count separation and QL is the mapping-induced residual count contribution. The corresponding continuum line element is obtained through coarse-grained realization,
establishing the connection between realized count separation and the emergent metric description.
The metric may therefore be expressed as the coarse-grained second-order response of the count resolved separation functional,
providing an explicit bridge between discrete count structure and continuum geometry. Using the count coordinate correspondence
the metric becomes
The associated connection coefficients are therefore determined by the same count-resolved structure,
and inherit their form from the realized metric rather than from an independently postulated spacetime geometry. The resulting curvature tensors follow the standard differential geometric construction,
Thus, the metric, connection, and curvature arise as successive realizations of count-resolved separation under the Frames mapping. Equations (43–51) make this dependence explicit, demonstrating how the standard geometric structures of gravitation emerge from the same count-based kinematic framework that governs the realized physical descriptions obtained from MQ. This establishes the geometric description of MQ as a consequence of Internal Frame count structure while preserving the conventional continuum formulation used in gravitational physics [2,18].
3.3.3 Geodesic Dynamics from the Same Action
Particle dynamics in the gravitational limit follow directly from the same MQ action functional (Sec. 3.1). The distinction between electromagnetic and gravitational behavior arises solely from how the Frames mapping is evaluated across count separation. In the continuum encoding, trajectory evolution is governed by the effective geometric structure induced by the coarse-grained encoded availability field ρR and the emergent metric
(Sec. 3.3.2). The action is therefore understood as the evaluation of the MQ action along an admissible trajectory xμ(λ), with λ an affine parameter consistent with the variational structure (Sec. 3.1.1). Variation of this action with respect to admissible trajectory perturbations yields the Euler–Lagrange equation
which is identical in form to the variational structure obtained in Appx. E (Eqs. E.4–E.8), where the covariant divergence and volume-form identities yield the Euler–Lagrange condition under admissible variations of encoded availability. This establishes that the trajectory equations here are not independently introduced but are the direct specialization of the general MQ variational principle under coarse-grained evaluation of the Frames mapping. Upon rearrangement using metric compatibility, Eq. (52) takes the standard geodesic form
where the effective connection coefficients are given by
These equations demonstrate that geodesic motion is not introduced as an independent postulate but follows from extremization of the MQ action after coarse-graining of conserved count structure after the Frames mapping has induced the effective metric
and its associated connection. Because
is derived from coarse-grained Internal Frame count structure rather than assumed as a primitive spacetime object, the connection coefficients
inherit their form from the same underlying adjacency relations. Curvature and trajectory evolution therefore arise from a common count-based origin within the Frames mapping.
This establishes that the geometric description of gravitation – traditionally introduced through an independent spacetime metric – is recovered here as a secondary construct arising from count-based kinematics. The resulting structure is formally equivalent to the geodesic formulation of GR [2,18], but differs fundamentally in that both the metric and the connection are derived rather than postulated.
Importantly, this derivation closes the unification loop. The same MQ action functional governs both electromagnetic and gravitational behavior without the introduction of independent dynamical structures. The observed distinction between interactions is therefore not fundamental but reflects how a single underlying Frames mapping is evaluated at a fixed interaction count in the electromagnetic case and across continuous count separations in the gravitational case.
3.3.4 Emergent Gravitational Coupling from MQ Scaling
The gravitational coupling constant G is not introduced as an independent parameter but arises from Frames mapping normalization of Internal Frame count structure into the System Frame, with its effective value determined by count-dependent contraction governed by the Informativity differential 2QLnL (Secs. 3.3.1–3.3.3). At the level of MQ primitives the normalization of geometric response yields
where the dependence on lf, mf, tf and 2QLnL is explicit and derived directly from the count-based action (Sec. 3.1). This result aligns with an electromagnetic determination of G as recommended in the 2010 CODATA publication [19]. The role of the contraction term is now made precise (Sec. 3.1.2). For gravitational interactions, often measured at macroscopic separations, the contraction term rapidly approaches its upper bound with no contribution to an observable variation,
Consequently, gravitational coupling appears constant in macroscopic measurements, consistent with time-of-swing determinations discussed in the 2014 CODATA publication of G [20]. The coupling constant is therefore understood not as fundamental, but as the large-count limit of a more general MQ scaling relation. Notably, within MQ, we do not italicize terms resolved at the upper count limit. All other terms are italicized, as is the practice for any measured variable.
This behavior contrasts with the electromagnetic realization, where interactions occur at the fixed count separation defined by the electromagnetic demarcation, nL=84.60055lf (Eq. 31). At this count, the non-Lorentz length contraction remains significant. Electromagnetic interactions therefore probe a fixed finite-count separation within the mapping, while gravitational interactions correspond to larger separations for which the contraction approaches unity. Distinction between coupling structures arises from count separation within the same underlying Frames mapping.
The same normalization procedure extends directly to the scalar structure governing large-scale expansion. Defining the geometric scalar through the MQ scaling relation ([9], Appx. BB) and the System Frame representation of the Hubble constant ([22], Eq. 84), respectively
one obtains
which links the effective cosmological term to the same count-based normalization that determines gravitational coupling. In this formulation, the cosmological contribution is not an independent parameter, but a direct consequence of geometric scaling under the Frames mapping. This establishes that both gravitational coupling and cosmological dynamics arise from a single kinematic origin. The distinction between local gravitational interaction and global expansion is therefore not fundamental but reflects different manifestations of the same normalization structure applied across scales.
Importantly, because the contraction term becomes nontrivial only at small count scales, MQ predicts that deviations from constant G should appear only at count separations approaching the electromagnetic demarcation. At macroscopic distances, the suppression of 2QLnL ensures agreement with classical gravitational measurements, while at short distances the framework allows for systematic, albeit small, deviations tied directly to the underlying discrete measure structure.
3.4 Unified Symmetry and Consistency Structure
The preceding sections established that the MQ action yields both the fixed-count electromagnetic realization and the coarse-grained geometric gravitational description as count-dependent realizations of a single underlying Frames mapping. The remaining requirement for unification is internal consistency. The framework must show that the source structure, conservation relations, and gauge compatibility of these emergent descriptions arise from the same variational origin rather than being imposed independently.
In MQ, this requirement is especially stringent because none of the central continuum objects are fundamental. The effective metric descriptor, the associated connection structure, and the encoded matter variables all arise only after admissible coarse-graining of Internal Frame count structure into a System Frame representation. It follows that any acceptable stress–energy definition, conservation statement, or gauge consistency condition must be formulated with respect to these emergent descriptors and must remain subordinate to the admissibility conditions of the Frames mapping itself. Those admissibility conditions – normalization, unique realization, and holonomy-free closure on admissible cycles – were already introduced as part of the variational structure and remain the governing constraints here.
Accordingly, this section does not introduce three disconnected consistency principles. Rather, it shows that the MQ framework supports a single consistency structure with three mutually linked manifestations. First, variation with respect to the emergent metric descriptor defines the appropriate stress–energy response object for the geometric realization. Second, invariance of the effective action under admissible geometric reparameterizations yields the corresponding covariant conservation law. Third, compatibility of the derivative structure with the same action guarantees that gauge structure does not conflict with the emergent energy–momentum description.
The purpose of the present section is therefore limited and precise. It is not to reconstruct the full gravitational field equations, nor to anticipate the parameter-reduction program of Sec. 3.5. Instead, the goal is to demonstrate that once the effective geometric realization has emerged, the MQ framework retains the same level of structural discipline expected of any viable unified theory: a well-defined source term, a conservation law derived from invariance, and consistency between geometric and gauge descriptions. In this way, Secs. 3.4.1–3.4.4 complete the logical transition from emergent dynamics to unified consistency, thereby preparing the ground for the parameter-reduction analysis that follows.
3.4.1 Stress–Energy from Metric Variation
Within MQ, the analogue of stress–energy is defined only after an admissible Frames mapping has produced an effective local System Frame relational descriptor
. This object is not fundamental. It is the emergent symmetric rank-2 descriptor encoding local relational geometry induced from Internal Frame count structure. Its role parallels the metric in GR, but its ontological status differs. It is not a primitive field but a derived encoding of count geometry [2,18,26,27]. Let the matter action be written as
where ψ denotes the encoded non-geometric fields arising from the Frames mapping, and ℛ is the admissible System Frame region corresponding to a mapped subset of the Internal Frame configuration domain. The dependence on
is entirely induced through the mapping and its associated covariant structure.
Variation is taken with respect to admissible deformations of
generated by the Frames mapping. These variations are constrained to preserve normalization, unique realization, and holonomy-free closure, ensuring that the perturbed configuration remains within the admissible class defined by the MQ variational principle. The first variation of the matter action defines the MQ stress–energy tensor,
which yields the explicit definition (Appx. E)
This equation is the MQ analogue of the Hilbert definition of stress–energy. It defines the response of encoded matter to admissible variations of the emergent relational geometry. Importantly, the variation is not applied to a fundamental spacetime field, but to a descriptor induced by the Frames mapping. Thus, Tμν measures the sensitivity of encoded matter to changes in the mapping-induced geometry rather than to perturbations of a primitive continuum background. Because the variation is taken with respect to a symmetric rank-2 descriptor, the resulting tensor is symmetric, Tμν=Tνμ. This symmetry is not imposed but follows directly from the structure of admissible variations.
The validity of Eqs. (61,62) and the upcoming Eq. (63) require that the matter action depends on
only through the induced covariant structure and not through independent derivatives of the metric treated as separate matter variables. Under this condition, the tensor defined above is the unique symmetric response object appropriate for the emergent gravitational realization [18,26,27,28].
For completeness, the same construction may be written at the level of the effective action density (Appx. E). When the encoded matter Lagrangian takes the local form ℒℳ𝒬, the stress–energy tensor admits the equivalent explicit representation
This form does not introduce a new definition. It is the local density form of Eq. (62) and makes explicit how the encoded matter responds to admissible metric variation in the emergent System Frame description.
The conceptual distinction from GR is therefore precise. In GR, stress–energy arises from variation with respect to a fundamental spacetime metric. In MQ, the identical variational structure is retained, but the varied object is an emergent descriptor derived from Internal Frame count geometry. This preserves the mathematical structure of the Hilbert construction while replacing its ontological foundation.
The conservation law associated with this definition is not assumed here. It follows from invariance properties of the effective action under admissible transformations of the emergent geometry and is derived explicitly in Sec. 3.4.2, consistent with the MQ analogue of Noether’s theorem developed in Sec. 3.2.2 [15,28].
3.4.2 Covariant Conservation from Diffeomorphism Invariance
This section establishes that the conservation structure associated with the MQ action is fully consistent with the covariant conservation laws of continuum field theory. The expressions presented below follow the standard variational treatment of diffeomorphism invariance and are included primarily to demonstrate that no additional assumptions or inconsistencies arise when the Frames mapping is evaluated in its coarse-grained geometric form. In particular, the resulting conservation law is not introduced independently but follows directly from admissible variations of the MQ action, ensuring compatibility with the established geometric formulation while preserving the count-based origin of the framework. The equations are therefore provided for completeness and reference, rather than as new structural input.
3.4.2.1 Variation of Fields under Diffeomorphism Invariance
Consider an infinitesimal diffeomorphism generated by a smooth vector field ξμ defined on the System Frame realization ℛ. The corresponding infinitesimal coordinate transformation is
the associated co-vector defined by
. The induced variation of the emergent metric is then given by the Lie derivative in covariant form,
where ∇μ is the Levi–Civita covariant derivative compatible with
.
Crucially, admissibility in MQ requires that ξμ generate deformations that preserve normalization of the Frames mapping, unique realization, and closure consistency on contractible reference cycles. Thus, Eq. (65) represents not an arbitrary coordinate variation, but the System Frame encoding of admissible Internal Frame deformations.
To connect this admissible diffeomorphism-induced variation with the MQ variational definition, Eq. (65) provides a restricted but sufficient class of metric variations for evaluating the action variation in Eq. (61). Substituting the induced variation into Eq. (61) and using the definition of Tμν in Eqs. (62–63), the resulting variation depends linearly on ξμ. Integration by parts transfers derivatives onto Tμν, yielding a divergence term proportional to ∇μTμν. Since ξμ is arbitrary within the admissible class, invariance of the action under these transformations implies ∇μTμν=0, establishing the conservation law within the MQ variational framework.
The invariance considered here must be interpreted consistently with the MQ variational framework. In contrast to GR, where diffeomorphism invariance is defined over arbitrary smooth variations of the metric, the MQ action is varied only over admissible configurations generated by the Frames mapping. These variations are constrained to preserve normalization, unique realization, and holonomy-free closure, as established in Appx. B. However, this restriction does not weaken the invariance argument. The admissible variations form a closed class under infinitesimal transformations of the emergent System Frame geometry and therefore include the subset required to generate the conservation identity. In this sense, diffeomorphism invariance is not imposed as an independent symmetry but arises as the effective invariance of the emergent geometric descriptor under admissible mapping-induced deformations.
3.4.2.2 Variation of the Action
Variation of the matter action under this transformation as presented in Eq. (61) is
Substituting the admissible diffeomorphism-induced metric variation from Eq. (65), and using the symmetry of Tμν, one obtains
where index lowering is performed with
. The reduction to Eq. (67) and the covariant integration-by-parts step leading to Eq. (68) follow from standard identities associated with metric compatibility and are derived explicitly in Eqs. E.4–E.9. Substituting Eq. (65) yields
Applying covariant integration by parts and using metric compatibility,
where boundary terms vanish under standard compact-support or asymptotic falloff conditions.
3.4.2.3 Covariant Conservation Law
Diffeomorphism invariance requires δSMQ=0 for arbitrary admissible ξμ. Therefore,
This is the MQ covariant conservation law. Its formal structure matches that of GR [18,24], but its interpretation differs fundamentally.
3.4.2.4 Internal Frame Origin and Continuum Realization of Conservation
In MQ, Eq. (69) is the realized System Frame representation of an underlying Internal Frame count conservation law defined over relational regions ω'⊂ω (Appx. K). The primitive Internal Frame quantity is the discrete measurement availability count nI(ξ,A), where ξ labels a relational cell and Ais the Internal Frame update index. The regional count is defined as
The conservation law is fundamentally relational and takes the form of an adjacency-balance relation between the local count nI(ξ,A) and the adjacency count-flux JI, defined on oriented relational links of the configuration domain ω. At the relational-cell level,
Summing Eq. (72) over all ξ∈ω'yields the regional conservation law
where ∂ω'denotes the adjacency boundary and ϕI(∂ω',A)is the Internal Frame boundary count-flux,
Using Eq. (71), Eq. (73) may be written compactly as
For closed relational regions satisfying
the total Internal Frame count is conserved,
Only after application of the Frames mapping does this conservation structure admit a realized System Frame continuum representation. Under that realization, the conserved Internal Frame count induces an encoded availability density ρS(r,t) together with the corresponding realized conservation relations of the System Frame. The continuum continuity relation therefore belongs to the realized System Frame, while Eqs. (67–73) remain the primitive discrete conservation structure from which that continuum representation is derived.
The conservation laws appearing in the realized System Frame are not independent postulates. Rather, they arise from the realization of conserved Internal Frame count under the Frames mapping and the associated mapping normalization functional. The discrete adjacency-balance relation of Eq. (73) therefore provides the primitive conservation statement, while the continuum conservation laws represent its realized geometric encoding.
Within the continuum description, conservation is expressed through the stress–energy tensor Tμν, whose covariant conservation follows from the metric realization of the MQ action and the diffeomorphism invariance of the emergent geometric description. The resulting conservation law is
Equation (78) is therefore the realized System Frame expression of conservation, whereas Eqs. (62–68) describe the underlying Internal Frame count conservation from which that continuum relation ultimately derives. Covariant conservation in the System Frame is thus the continuum realization of conserved count under the Frames mapping. Equation (72) provides the primitive adjacency-balance condition, while Eq. (78) represents the corresponding conservation law in the emergent metric description.
3.4.2.5 Significance
As established by Eqs. (72–78), the discrete adjacency conservation law of the Internal Frame is carried into the continuum as the covariant conservation statement ∇μTμν=0. Thus, Eq. (72) is the continuum image of count conservation, while the discrete adjacency relations in the Internal Frame provide the fundamental kinematic origin.
The result places covariant conservation precisely within the logical structure of the framework. It follows from the stress–energy definition (Sec. 3.4.1), precedes gauge structure (Sec. 3.4.3), and ensures compatibility with established relativistic field theory while eliminating the need for an independent conservation postulate. Accordingly, MQ reproduces the conservation structure required by modern field theory [15,18,24], but reinterprets it as a consequence of the Frames Principle applied to a discrete count-based substrate.
3.4.3 Gauge Invariance of the Energy–Momentum Tensor
At the fixed interaction count defined by the electromagnetic demarcation, where the mapping-induced normalization is constant (Sec. 3.2), the emergent Abelian gauge structure is encoded in the System Frame through a potential field defined on the realized relational structure. Gauge transformations correspond to reparameterizations of this encoded representation,
where χ is a scalar field on the System Frame. Under this transformation, the field strength tensor becomes
demonstrating invariance under Abelian gauge transformations through the commutativity of partial derivatives. Observable gauge quantities must therefore be constructed from the gauge invariant field tensor Fμν together with the emergent metric descriptor
, consistent with standard gauge invariant field theory [15,17,18,27].
Let the gauge contribution to the MQ Action be defined as the realization of the action at the fixed interaction distance corresponding to the electromagnetic demarcation in the System Frame,
such that the MQ Action admits distinct realizations determined by count separation under the Frames mapping. In this formulation, the gauge contribution corresponds to evaluation at a fixed interaction distance, while gravitational behavior corresponds to count-resolved realizations in which the same action yields an effective metric structure in the System Frame.
The associated stress–energy tensor (Sec. 3.4.1) is obtained through variation with respect to the emergent metric descriptor,
Because ℒgauge depends on 𝒜μ only through the gauge invariant tensor Fμν, its variation under the transformation (79) vanishes identically. It follows directly that
This establishes that the energy–momentum tensor derived from the MQ action is gauge invariant without requiring an independent postulate. In local density form, for a gauge invariant Lagrangian depending only on Fμν and
,
Thus, the stress–energy tensor may be written equivalently as
Since the Lagrangian depends only on the gauge invariant field strength, the tensor inherits gauge invariance directly,
. This is not an independent definition, but the explicit local realization of the variational statement in Eq. (82).
Within the MQ framework, gauge invariance must be interpreted at the correct structural level. Gauge transformations are not symmetries of the Internal Frame, which is governed by discrete count structure and the Frames mapping, but arise only after encoding into the System Frame, where derivative-based representations become admissible. They express that distinct System Frame encodings related by 𝒜μ→𝒜μ+∂μλ correspond to the same underlying count configuration. Observable quantities are therefore restricted to invariant combinations, and the stress–energy tensor inherits this invariance directly. Gauge symmetry is thus a redundancy of representation, not a fundamental symmetry of the Internal Frame.
Therein, the MQ action satisfies co-emergent consistency conditions: metric variation yields the stress–energy tensor (Sec. 3.4.1), diffeomorphism invariance yields covariant conservation (Sec. 3.4.2), and gauge invariance ensures an invariant energy–momentum tensor. These are not imposed independently but arise from a single underlying action defined on the MQ kinematic substrate. Electromagnetic gauge structure, gravitational stress–energy response, and conservation laws therefore emerge as unified consequences of the same count-based action principle, establishing internal consistency across all symmetry structures required for unification.
The gauge invariant form of
has a direct consequence for the coupling structure of the unified theory. Because the stress–energy tensor is obtained entirely from variation of the same MQ action, no independent coupling parameter is introduced at the level of the electromagnetic interactions. All coupling information is therefore encoded through the Frames mapping and the emergent metric descriptor
. The source term entering the gravitational limit is therefore obtained from the same unified functional,
where SMQ contains both derivative- and curvature-dominated contributions determined by count separation. Because the electromagnetic contribution satisfies
, the source entering the emergent gravitational description inherits gauge invariance automatically. Thus, no additional compatibility condition between electromagnetic and gravitational descriptions is required: both arise from a single variational structure. This establishes that the absence of independent coupling constants is not an imposed constraint, but a structural consequence of the MQ action.
3.4.4 Why these Structures Matter for Unification
The results of Secs. 3.4.1–3.4.3 establish a single closed consistency chain within the MQ framework: variation of the MQ Action with respect to the emergent geometric descriptor yields the stress–energy tensor (Appx. E.2.3–E.2.4), invariance under admissible diffeomorphic deformations – enforced by holonomy-free closure on contractible cycles – yields covariant conservation (Appx. E.3.1–E.3.2), and invariance of the derivative-based action under Abelian gauge reparameterization – arising from admissible re-scalings of encoded availability – leaves the corresponding energy–momentum tensor unchanged (Appx. E.2.5). As emphasized at the conclusion of Sec. 3.4.3, all contributions to the stress–energy tensor arise from a single MQ Action, so that symmetry, conservation, and sourcing are not independently specified but share a common variational origin.
The significance of this chain lies in the fact that these structures are not introduced independently but arise from a single underlying condition: the admissibility of the Frames mapping between the Internal and System Frame.
In conventional continuum formulations, these structures are implemented through formally distinct mechanisms. The stress–energy tensor is obtained by variation of the matter action with respect to a metric, covariant conservation follows from diffeomorphism invariance, and gauge invariance is imposed through symmetry of the relevant field description. These constructions are mutually consistent but logically independent. In contrast, within MQ, all three arise from the same kinematic requirement: that the Frames mapping preserves normalization, ensures unique realization, and admits holonomy-free closure on contractible cycles. This relocation of structure eliminates a layer of independently specified structure that has historically obstructed unification [15,18,27,28].
The preceding subsections further show that both the emergent geometric realization and the emergent Abelian gauge structure are derived from the same action functional defined on the MQ substrate. The gravitational limit is obtained when the coarse-grained mapping admits an effective geometric description, yielding dynamics consistent with geodesic motion and metric variation. The electromagnetic limit is obtained in the electromagnetic demarcation, where the admissible encoding produces an Abelian gauge structure governed by the field strength tensor. The critical point is that these structures are not constructed separately and later combined; rather, they are different realizations of the same variational structure relative to the count distance. This establishes that the apparent distinction between geometric and gauge interactions is not fundamental but emergent from a deeper kinematic origin [17,18,24,29].
A direct consequence of this unified origin is a restriction of admissible theory space. Because stress–energy, conservation, and gauge invariance must all arise from the same Frames mapping, any candidate realization that violates normalization, uniqueness, or closure conditions cannot produce a consistent physical theory within MQ. Thus, the framework does not expand the space of allowable models through independent structural freedoms; instead, it constrains that space by requiring that all interaction descriptions satisfy a single set of kinematic admissibility conditions. This constraint-driven structure is a defining feature of a viable unification framework, as it prevents agreement in one description from being obtained at the expense of inconsistency in another [15,17,18,30].
The broader implication is that the familiar symmetry structures of continuum physics – gauge invariance and diffeomorphism invariance – are not fundamental postulates within MQ but emergent properties of the encoded System Frame. The underlying ontology resides in the discrete count structure of the Internal Frame, with the Frames mapping acting as the mechanism through which continuum representations arise. In this sense, MQ does not unify pre-existing theories by imposing additional symmetries or higher-dimensional constructs, as in Kaluza–Klein or string-theoretic approaches [3–7]. Instead, it derives both geometric and gauge structures from a single kinematic substrate, shifting the unification problem from external synthesis to internal derivation [18,24,29,31].
For the purposes of the present section, the unificatory content is therefore precisely defined. MQ establishes that the stress–energy tensor, its covariant conservation, and gauge invariance of the energy–momentum tensor all arise from one variational principle applied to a single count-based kinematic structure. This does not yet exhaust all aspects of gravitational and electromagnetic phenomena, but it provides the minimal structural closure required of any candidate unified theory: a common origin for the symmetry and conservation principles that govern both interaction descriptions.
3.5. Internal Frame Origin of Continuum Conservation Laws
In conventional formulations, gravitational and electromagnetic interactions are specified by independent constants introduced axiomatically, including G, e, and ħ. These constants are not derived from a common structure and therefore represent independent inputs to the theory. In MQ, the relevant conservation structure is defined first within the Internal Frame through discrete count measures and adjacency relations, together with the Frames mapping M:ω→R, which induces the realized System Frame representation. The distinct interaction behaviors observed in the continuum arise as different realizations of this underlying count structure, governed by the invariant parameter θsi introduced in Sec. 2.2.
The key structural result is that covariant conservation in the System Frame is not a primitive postulate, but the mapped realization of count-conserving relations defined on the Internal Frame. Let nI(ξ,A) denote the Internal Frame discrete count at relational cell ξand update index A. The corresponding regional count is
At the discrete level, conservation is expressed as an adjacency-balance relation between the local count and the adjacency count-flux. This relation is defined purely on the relational adjacency structure and carries no geometric or directional interpretation in the continuum sense, consistent with the Internal Frame definitions. At the relational-cell level,
Summing Eq. (88) over the relational region ω'⊂ω gives the regional conservation law
where ∂ω' denotes the adjacency boundary of ω', consisting of admissible adjacency links connecting relational cells inside the region to cells outside the region. The quantity ϕI(∂ω',A) is the Internal Frame boundary count-flux,
representing the exact net outward transport of measurement availability across the adjacency boundary. This quantity is a discrete count-flux defined entirely on the relational adjacency structure of the Internal Frame. It is not a geometric surface integral and carries no dependence on metric structure, coordinate systems, normal vectors, or continuum geometry.
Using Eq. (87), the regional conservation law immediately implies
Equation (91) states that when no net count-flux crosses the adjacency boundary, the total measurement availability contained within the relational region remains invariant under Internal Frame evolution. Regional conservation therefore follows directly from the local continuity relation and the adjacency-flux structure without introducing any geometric assumptions.
Equations (87–91) are entirely Internal Frame statements. They describe conservation of discrete measurement availability through redistribution of count across the relational adjacency structure. The quantities nI, NI, JI, and ϕI are count-based objects defined exclusively on the relational domain ω, while divadj is a combinatorial operator acting on admissible adjacency transfers. No continuum density, coordinate system, geometric current, surface integral, or differential manifold structure is required.
Only after application of the Frames mapping does this conserved count structure admit realization within the System Frame. Under mapping normalization, conserved count, adjacency flux, and regional count transport are realized as continuum quantities defined on the realized relational structure Ω=M(ω'). The resulting continuum conservation relations therefore do not constitute independent postulates but arise from the realization of conserved Internal Frame count under the Frames mapping. In this sense, conservation in the realized System Frame is inherited directly from the discrete conservation structure encoded by Eqs. (87–91).
The corresponding continuum representation supplies the conservation structure required by the MQ Action and the MQ variational principle. In the realized continuum description, mapping-normalized count conservation induces the conserved current structure associated with encoded availability and yields the covariant conservation condition satisfied by the emergent stress-energy tensor, ∇μTμν=0.
This relation is therefore not imposed at the primitive count level. Rather, it is the realized System Frame conservation law obtained through application of the Frames mapping to the underlying discrete conservation structure of the Internal Frame.
3.5.1 Mapping of Interaction Structure
This section establishes that all interaction structure originates from a single invariant count parameter and the conservation laws of the Internal Frame. Specifically, the absence of independently introduced coupling constants implies that interaction strength is determined by the same invariant parameter governing the Frames mapping. In MQ, this role is played by the dimensionless parameter θsi, which controls the discrete-to-continuum realization of admissible configurations.
Dependence enters through the normalization of conserved flux under the mapping. For electromagnetic interactions, this normalization yields a fixed interaction distance at the electromagnetic demarcation. For gravitational phenomena, the same conserved quantity is realized at the relative distance between two phenomena (Appx. D). In both cases, interaction strength is determined by count-resolved realizations of the same conserved structure. Thus, both interaction strengths arise from a common relation governed by θsi, with their distinction reflecting different realizations of the same conserved structure under the Frames mapping.
Because interaction strength is fixed by the normalization, the effective couplings are not free parameters (Appx. F). Independent constants are reduced. This reduction imposes cross-domain constraints, whereby measurements in one interaction realization restrict the admissible realization of others, providing a necessary condition for unification within MQ. Explicit derivations of standard physical constants are given in Appx. H.
3.5.2 Geometric Origin of Coupling Structure
The relation between gravitational and electromagnetic quantities in MQ follows from the common normalization structure governing realized fields in the System Frame. No independent coupling constants appear at the level of the MQ Action,
and all interaction structure arises from the realization of invariant count relations under the Frames mapping.
The passage from discrete count structure in the Internal Frame to continuum quantities in the System Frame is governed by the mapping normalization functional (Secs. A.3, A.7). This functional maps admissible regional counts NI(ω',A) into a normalized continuum measure, from which the encoded availability density ρℛ is defined, enforcing conservation and realization consistency while providing the operative link between invariant count measures and the realized field quantities entering Eq. (92). No additional degrees of freedom are introduced.
Within this structure, electromagnetic and gravitational quantities correspond to distinct realizations of the same normalized count substrate. For electromagnetic interactions, normalization occurs at the electromagnetic demarcation, where the count separation nL = 276/θsi, sets the fixed interaction scale and thereby determines the scale of the emergent Abelian gauge structure. For gravitational interactions, the same normalized count structure is realized through coarse-graining, yielding the effective metric
and its associated geometric scaling (Sec. 3.3.4, Appx. D). Accordingly, both phenomena are linked through their dependence on θsi and the normalization structure of the Frames mapping. Their distinction is realized as a function of count separation.
The Internal Frame provides the invariant count substrate, while the System Frame realizes measurable quantities through normalization. The discrete count separation nL, defined as the count of lf between a system and a center of mass, characterizes the realized interaction scale, but it should be noted that each is a distinct realization of the Frames mapping. As a consequence, constants associated with electromagnetic and gravitational interactions do not appear independently at the level of the action. Electromagnetic quantities arise from boundary-flux normalization at the fixed count separation nL, while gravitational quantities arise from curvature scaling of the same normalized count structure. Both are determined by the invariant parameter θsi through the normalization functional. This establishes that the relation between gravitational and electromagnetic quantities in MQ is not a reduction of one interaction to the other, but the elimination of their independence at the level of first principles.
3.5.3 Fundamental, Realized, and Direct Measurement of Phenomena
The distinction between fundamental and directly measured quantities follows from the Frames Principle, which asserts that all observables arise through the Frames mapping from the Internal Frame to the System Frame . Fundamental measures are defined within the Internal Frame as invariant count-based quantities, while experimentally accessible values correspond to their realized forms in the System Frame. The mismatch between these values is therefore not anomalous, but a direct consequence of mapping-induced realization.
The MQ fundamental measures are resolved in Ref. ([9], BN5, BN7, and BN10),
Notice, that both ħ and G are not italicized indicating that we should use the macroscopically determined value for G as found in the 2014 CODATA publication and the calculated value for ħ as resolved at the upper count limit. Multiplying Eq. (93) by Eq. (95) gives
and multiplying Eq. (94) by Eq. (95) gives
These results show that the MQ fundamental measures satisfy the identities
The result is structurally significant. The Compton-form relations emerge directly from the MQ fundamental definitions without introducing any additional assumptions. In standard treatments, the Compton wavelength is defined with respect to a particle mass introduced independently. Here, the same structure arises as a necessary identity of the fundamental measures themselves, demonstrating that Compton-scale relations are intrinsic to the MQ kinematic framework.
The transition to experimentally accessible quantities follows from realization in the System Frame. As established in Appx. A, all observables are defined only after mapping and normalization . Consequently, the physically realized description is determined by the mass scale at which measurement is instantiated. For electromagnetic observations, this description is defined by the electron mass me. Substituting the realized mass scale me into Eqs. (98–100) yields the realized Compton relations
These relations define the first directly accessible length and time scales associated with electromagnetic measurement and correspond to the reduced Compton scale of the electron [32]. The appearance of the electron mass reflects the realized measurement scale imposed by the interaction count [50,51], consistent with the definition of the electromagnetic demarcation.
Table III: Fundamental, Realized, and Directly Measured Quantities [33,34] | ||||
Quantity | Fundamental | Realized (macro) | Realized (EM) | Direct Measured |
Mass (kg) | 2.17643254 × 10-8 | 9.1093837139 × 10-31 | 9.1097018900 × 10-31 | 9.1093837139(28) × 10-31 |
Length(m) | 1.616255 × 10-35 | 3.861457800 × 10-13 | 3.861592674 × 10-13 | 3.7(1) × 10-13 |
Time (s) | 5.391247 × 10-44 | 1.288043677 × 10-21 | 1.288088666 × 10-21 | -- |
Evaluating these expressions using the measured electron mass yields the realized quantities reported in Table III, with the “Realized (EM)” calculations corresponding to the electromagnetic determination of me [33]. Notably, the directly measured displacement ldirect is consistent with the predicted realized length lrealized [34] within experimental uncertainty.
Importantly, this analysis addresses the observation that fundamental mass is many orders of magnitude larger than directly measured phenomena such as the mass of the electron. Since the fundamental measures satisfy lfmf = 2θsitf, it follows that determination of a length larger than the smallest realizable length must be correlated with a mass larger than the smallest realizable mass. The true minimal measurable values for these quantities, however, remain experimentally unresolved.
The notion of a smallest measure is complicated by the Frames mapping process. Notably, fundamental measures are mapping constructions between the Internal and System Frame representations of the three dimensions. Up to this point, the mapping – identified through the metric differential – differs across the resolved physical constants. Because of the fundamental role of three-dimensional structure, it remains unclear whether the mapping values correspond directly to minimal realizable measurements in the System Frame or instead reflect normalization relative to those minima. In this sense, the metric differential has not been uniquely fixed. The Compton scale may provide guidance in this direction, but at present the analysis identifies structural constraints rather than definitive minimal values.
3.5.4 Relation of Gravitational and Electromagnetic Quantities through θ
The invariant scalar θsi organizes the relation between invariant count structure and measurable physical quantities. It is invariant under Internal Frame representation while admitting distinct dimensional realizations under System Frame encoding.
3.5.4.1 Electromagnetic Realization: Explicit Dependence
The dependence of electromagnetic quantities on θsi is explicit within the MQ term structure. By example, the inverse fine structure constant is given by ([9], Appx. AA)
This expression follows directly from the count-based structure of the Internal Frame and its realization under the Frames mapping [19,25,35]. It establishes that a quantity conventionally treated as an independent coupling constant is fully determined within the MQ framework by the invariant scalar θsi. The same scalar defines the electromagnetic demarcation nL = 276/θsi, where nL is the count of fundamental lengths lf between a system and a reference center of mass. Together, Eq. (104) and the definition of the electromagnetic demarcation establish that the electromagnetic interactions corresponds to a fixed realization of θsi at a specific count scale, while ∇μTμν=0 (Eq. 78) gives the covariant conservation law satisfied by the corresponding stress–energy tensor.
3.5.4.2 Gravitational Realization: Mapping-Dependent Realization
Gravitational behavior is governed by the same invariant scalar θsi, but its realization differs fundamentally from the electromagnetic case in that it is not associated with a fixed interaction scale. Instead, gravitational observables emerge through mapping-dependent realization over a relational separation characterized by the count distance nL.
In MQ, no independent gravitational constant is introduced at the level of the action. Gravitational coupling arises from the normalization of Internal Frame count structure under the Frames mapping, together with the scaling behavior induced by relational separation. This leads directly to a mapping-dependent realization of the gravitational coupling ([9], Appx. C, D)
where 2QLnL encodes the Informativity differential and nL denotes the count separation between the realized system and the associated center of mass. This expression follows directly from the MQ scaling relations.
Unlike electromagnetic interactions, which are characterized by a fixed interaction scale nL = 276/θsi, gravitational behavior admits realization over arbitrary count separations. Consequently, the effective gravitational coupling inherits an explicit dependence on nL. The conventional gravitational constant is recovered only in the asymptotic limit of large count separation. Taking the upper-count limit yields
demonstrating that the macroscopic gravitational constant is itself a derived quantity, fixed entirely by the MQ fundamental measures. This formulation also makes clear that gravitational coupling in MQ is not a universal constant in the conventional sense, but a realization-dependent quantity determined by θsi, the fundamental measures lf, mf, tf, and the relational count distance nL.
Accordingly, the apparent constancy of G in classical physics reflects the large-scale limit of the theory, while deviations at shorter count scales arise naturally from the underlying count geometry. This replaces the notion of a fundamental gravitational constant with a derived, scale-dependent quantity emerging from first principles MQ structure.
3.5.5 Comparison with Classical Formulations
Classical physics treats electromagnetism and gravitation as fundamentally distinct theoretical structures. Electromagnetism is formulated through Maxwell’s equations and the associated electromagnetic constants. Gravitation is formulated through Einstein’s field equations and the gravitational constant G [1,2]. In each case, the theory is introduced with its own primitive structure. This separation is part of the standard framework and is reflected both in the mathematics and in the independent status granted to the corresponding constants.
Within MQ, the comparison is different because these descriptions do not begin with separate primitives. As established in Secs. 3.5.1 and 3.5.2, both are resolved from the same Frames mapping, the same fundamental measures, and the same invariant scalar θsi. The contrast with the classical picture can therefore be stated precisely.
(i) Independence vs. derivation of constants
In the classical description, constants entering electromagnetic and gravitational theory are independent inputs. In MQ, by contrast, measurable quantities are resolved from the common count-based structure defined by the fundamental measures lf, mf, tf, the associated count structure nL and θsi. Equation (95) makes this explicit for the inverse fine structure constant. The point is not that every constant has already been rederived in this subsection, but that the framework no longer grants them independent foundational status.
(ii) Distinct vs. unified geometric structure
In GR, geometry is primary. In classical electromagnetism, the theory is formulated on a spacetime background through a gauge field description. MQ does not begin with either as a primitive structure. The Internal Frame, System Frame, and Frames mapping supply a single underlying kinematic structure from which different physical descriptions are realized. Thus, the classical duality of metric and field descriptions is replaced by a single relational substrate.
(iii) Scale separation vs. scale-dependent realization
Classically, electromagnetism and gravitation are distinct across all scales by construction. In MQ, the realized description depends on count separation. Electromagnetic interactions are tied to the fixed electromagnetic demarcation introduced in Eqs. (14–16) and expressed in Sec. 3.5.4 through nL = 276/θsi, whereas gravitational quantities are resolved relative to nL, the count distance to a center of mass. The distinction is therefore scale-dependent and count-dependent, not foundational. This is consistent with the role assigned earlier to count distance and contraction structure, while avoiding the introduction of any new derivation here.
(iv) Parameter proliferation vs. parameter reduction
Many unification programs extend the standard framework by adding dimensions, fields, or new independent parameters [3–8]. MQ proceeds in the opposite direction. It reduces the number of independent inputs by requiring that physical quantities be expressed through the same invariant count structure. In this respect, MQ does not merely re-describe two classes of physical behavior. It restricts admissible physical descriptions by denying them separate primitive origins.
(v) Conceptual implication
The conceptual implication is that the classical distinction between electromagnetism and gravitation is retained as an effective difference in realization, but not as a difference in foundation. In MQ, the distinction reflects how the Frames mapping resolves the underlying count structure in the System Frame under different conditions, not the existence of two unrelated primitive interactions.
3.6 Observable Structure of Coupling and Frame-Dependent Differentiation
A physically meaningful unification of gravitation and electromagnetism requires that each phenomenon be expressed in terms of a common set of physically distinct quantities whose definitions are independent of the phenomena being compared. The comparison must isolate the terms responsible for differences between the interactions such that these differences correspond to well-defined physical effects rather than independent coupling assumptions. To establish this, we consider the relationship between the gravitational constant G and the electric constant ɛ0. Given that the electric and magnetic constants satisfy ɛ0 = 1/(u0c2), it is sufficient to compare G and ɛ0.
Using the MQ representations for G and ɛ0 (Appx. F), we arrange both expressions such that dimensional terms appear explicitly and in comparable form, preserving the decomposition into fundamental measures and dimensionless factors,
Inspection of these expressions shows that the dimensional terms associated with the electric constant correspond directly to those describing gravitation when expressed in the same fundamental measure basis. The distinction between the two constants therefore resides entirely in the remaining dimensionless factors rather than in their dimensional structure. Applying the final substitution yields
The interpretation of this result requires care. The constant G, as observed in the System Frame, is not an intrinsic property of gravitation alone but reflects a distance sensitive realized measure arising from the Frames mapping. In contrast, the expressions entering the comparison above are constructed from Internal Frame quantities, where no geometric or metric structure is presupposed. The difference between the two descriptions is therefore attributable to the mapping between frames, not to independent physical parameters.
The remaining factors that distinguish gravitation from electromagnetism do not arise from independent coupling structure but from how conserved count is realized under the Frames mapping. The mapping itself introduces no physical distortion. It is a kinematic transformation relating Internal Frame count structure to its realization in the System Frame. The observable differences instead arise from two distinct consequences of this realization.
The first is the Informativity differential, which defines a non-Lorentz length contraction associated with the discrete count structure of the Internal Frame and is expressed through the quantity 2QLnL. This effect modifies the normalization of realized separations as a function of count scale. The second is gravitational curvature, which arises from the incremental loss of non-whole units of lf under successive updates of fundamental time. This curvature is not an independent dynamical field but a geometric feature of the Internal Frame count structure as realized in the System Frame. The term γF encodes the combined influence of these effects within the admissibility conditions imposed by the Frames Principle.
The preceding analysis establishes that observables inferred within the MQ framework depend on the interaction count through which they are realized, reflecting the role of count-dependent normalization under the Frames mapping. Quantities inferred through distinct interaction channels therefore need not coincide when evaluated under different realization conditions, even when referring to the same underlying observable. This provides the basis for the comparison developed in the following section.
3.7 Empirical and Phenomenological Signatures of Unification
The preceding section establishes that observables within the MQ framework depend on the interaction count through count-dependent normalization under the Frames mapping. In particular, the Informativity differential introduces a non-Lorentz length contraction that varies with count separation. This effect is realized in that electromagnetic interactions occur at a fixed count defined by the electromagnetic demarcation nL = 276/θsi while gravitational measurements reflect the realized separation of the configuration. The effect is therefore realized through the comparison of measures using these two approaches.
A direct consequence is that quantities traditionally treated as universal constants acquire a dependence on interaction channel through their realization. In particular, the gravitational constant, when inferred through electromagnetic calibration, will differ from values obtained through purely gravitational measurements. With MQ, we distinguish this difference using the italic form of G to describe a value inferred at a finite count separation, while the non-italicized form corresponds to a value resolved in the upper-count limit. The inferred value is expressed as
showing explicitly that the measured value depends on the count-dependent factor 2QLnL. The effect appears in current high-precision measurements of G [36–39], which differ in the fourth significant digit across CODATA publications. Within the MQ concordance analysis, these discrepancies are clarified, with agreement reported at the 3.94σ level across CODATA publications for a common observable (Table I; Appx. H).
This behavior is further supported by the CODATA evolution analysis presented in Appx. G, where successive recommended values align closely with distinct MQ realizations. In particular, the 2010 and 2014 adjustments coincide with the finite-count and asymptotic branches, respectively, at residuals well below reported experimental uncertainties. While the CODATA procedure reflects statistical weighting over heterogeneous measurements rather than explicit selection of physical conditions, the observed alignment is consistent with the interpretation that different experimental methodologies sample distinct realizations under the Frames mapping.
For clarity, the magnitude of the Informativity differential increases with decreasing distance. This identifies electromagnetic interactions as the domain of highest sensitivity, while larger-scale systems probe conditions in which the effect is physically negligible.
This prediction is constrained and falsifiable. If measurements of G obtained through distinct interaction channels converge to a single value with increasing precision, or if no systematic cross-channel deviation is observed in inferred quantities, the mapping-dependent contribution would not be supported. It is therefore necessary to distinguish conventional scale dependence associated with dynamical interactions in the System Frame from mapping-induced effects of the Informativity differential. The former reflects interaction strength variation within a given realization, whereas the latter arises from the discrete-to-continuous mapping. Electromagnetic interactions, being fixed at the electromagnetic demarcation, do not sample variation in this contraction, while gravitational measurements encode its dependence on separation.
As macroscopic measurements have negligible difference, we find measurement of G will fall in one of two classes depending on the approach used:
These values correspond to realizations at the fixed electromagnetic demarcation and at the macroscopic limit.
These results show that a single kinematic structure yields multiple experimentally realized values of the same observable without introducing independent couplings. The electromagnetic interaction scale and gravitational coupling are therefore related through their dependence on the mapping structure governed by θsi. Cross-channel comparisons yield agreement at the 5.24σ level across independent implementations, reflecting consistency between distinct realizations rather than repeated measurements of a single observable (Table I; Appx. H).
All empirical and phenomenological signatures described here reduce to a common origin: the discrete count structure of the Internal Frame and its realization in the System Frame. The apparent diversity of physical behavior across electromagnetic and gravitational domains reflects interaction-dependent realization rather than distinct physical structures. The existence of multiple resolved values of G, linked through count distance as described by nL, provides a concrete and testable consequence of the MQ formulation.
4. DISCUSSION
4.1 What MQ Unifies
The MQ framework establishes a unification at the level of kinematics, rather than by postulating independent dynamical structures and subsequently attempting to couple them. Specifically, MQ demonstrates that both electromagnetic and gravitational phenomena arise from a single count-based substrate governed by the Frames mapping and constrained by the Frames Principle. Within this structure, distinctions between interaction types emerge not from fundamentally different fields, but from scale-dependent realizations of a common underlying action.
In classical formulations, electromagnetism and gravitation are described by structurally distinct theories – Maxwell’s equations defined on a fixed spacetime background [1,25,35], and Einstein’s field equations in which spacetime geometry itself becomes dynamical [2,23,24]. MQ replaces this dichotomy with a single relational construction in which the System Frame encoding arises from a deterministic mapping of Internal Frame count configurations. A single action functional governs the evolution, invariant across count separation, while observable behavior (Abelian gauge structure versus metric curvature) emerges through count-dependent reductions of this common structure.
The electromagnetic demarcation corresponds to count separations at which the derivative structure of encoded availability dominates, yielding an effectively Abelian gauge theory with conserved Noether currents [15,25]. The gravitational limit corresponds to coarse-grained descriptions in which accumulated count structure induces an emergent metric and geodesic dynamics [23,24]. These descriptions therefore represent distinct realizations of the same underlying kinematic structure.
Within this formulation, the invariant scalar θsi = lfmf/2tf governs the mapping between discrete counts and continuous observables and therefore sets the normalization of interaction strengths across count separation. Interaction scales follow directly from this structure: electromagnetic interactions are fixed by the electromagnetic demarcation nL = 276/θsi, while gravitational observables are determined by count-resolved separations under the contraction structure introduced in Sec. 2.3. This removes the need for independent coupling constants and provides a unified kinematic origin for electromagnetic and gravitational interactions (Secs. 3.5, 3.6.3).
A central consequence is the frame dependence of measured quantities. Independent tests of the contraction structure yield a concordance of 5.08σ, confirming that the Informativity differential is both structurally required and empirically realized across distinct realizations (Table I; Appx. H). The measured gravitational constant follows G = (2QLnL)c3(tf/mf), demonstrating that experimentally inferred values depend on the count scale at which the interaction is realized (Sec. 3.6.2). The distinction between electromagnetic-scale and macroscopic-scale realizations is therefore a direct consequence of the Frames Principle.
These results extend to observed experimental behavior. The CODATA evolution of the gravitational constant reflects shifts between statistically dominant measurement clusters that align with distinct MQ realizations (Appx. G), while cross-channel comparisons yield concordance across independent implementations (Table I; Appx. H). The MQ framework further reproduces observed cosmological expansion behavior within its kinematic formulation [22] and yields electromagnetic coupling values consistent with observation through Eq. (95). These agreements are obtained without introducing independent fit parameters, with the physical constants grouping achieving a concordance of 8.74σ (Table I; Appx. H).
Taken together, MQ provides a structural and constructive unification: a single generative mechanism from which both classical field theories arise as limiting descriptions, rather than a reconciliation of pre-existing formulations. Gauge interactions, geometric gravitation, discrete count kinematics, and continuum field descriptions are therefore unified as different realizations of a common underlying framework.
4.2 What the Present Paper Does Not Yet Claim
It is essential to delineate the scope of the present work to avoid overstating its conclusions. While the MQ framework establishes a unified kinematic origin for interaction phenomena and provides a set of concrete, testable predictions, it does not yet constitute a complete reconstruction of all known physical interactions or a finalized quantum theory of gravity. Its validity therefore rests not on interpretive consistency, but on whether the frame-dependent relations derived here are borne out under increasingly precise and cross-channel experimental conditions.
In particular, this work does not yet provide:
A complete experimental isolation of discrete contraction effects
The experimental isolation of the Informativity differential requires controlled multi-frame measurements at sufficiently small count scales, where deviations from classical expectations are maximized.
A systematic reanalysis of gravitational measurements under frame decomposition
Existing gravitational experiments must be reanalyzed under explicit frame decomposition to test the predicted structure of Eq. (112) across differing experimental methodologies.
A full renormalized quantum field theory embedding
Although the MQ framework produces a continuum limit with Schrödinger-type evolution and gauge structure, a complete treatment of renormalization and higher-order quantum corrections – analogous to the formal developments of effective field theory [12,13,40,41] – is deferred.
A full non-Abelian gauge generalization
The present treatment demonstrates emergence of an Abelian (Maxwell-type) structure. Extension to non-Abelian gauge symmetries (e.g., Yang–Mills [5]) requires further development of internal relational symmetries within the Frames mapping.
A complete cosmological solution space within the MQ action
While MQ provides scalar relations and expansion structure consistent with observational inference (as developed in prior work [22,42]), the full classification of cosmological solutions derived directly from the MQ action remains part of a subsequent program.
A finalized equivalence with General Relativity in all regimes
The present work demonstrates emergence of metric structure and geodesic dynamics, but a full equivalence proof – covering all strong-field and topologically nontrivial configurations – is deferred to a dedicated treatment.
Further development of the topological structure of the Frames mapping
The classification of mapping defects within the Frames Principle remains to be developed to determine how global structure constrains realized universes.
Accordingly, this paper should be interpreted as establishing the existence and internal consistency of a unified action-based framework, rather than presenting a completed end-state theory.
4.3 Position Relative to GR, Maxwell Theory, and Other Unification Attempts
The MQ framework occupies a distinct position relative to both classical field theories and historical unification efforts.
4.3.1 Relation to Maxwell theory
Maxwell’s formulation of electromagnetism represents one of the earliest successful unifications, combining electric and magnetic phenomena into a single field theory [1]. In modern form, this is understood as an Abelian gauge theory with local U(1) symmetry [25,35].
MQ reproduces this structure not by postulating gauge symmetry, but by deriving it as a consequence of the derivative-dominated evaluation of encoded availability at fixed count separation. Gauge invariance therefore emerges from the invariance properties of the Frames mapping, rather than being imposed axiomatically.
4.3.2 Relation to General Relativity
GR describes gravitation as curvature of spacetime induced by stress–energy [2,23,24]. Its geometric nature contrasts sharply with the gauge-theoretic structure of electromagnetism.
In MQ, this distinction is resolved: curvature is not fundamental, but emergent from coarse-grained count structure. The metric tensor appears as an effective description of relational encoding at large scales, while the underlying kinematics remains discrete and non-geometric. In this sense, MQ provides a pre-geometric substrate from which GR arises as an effective theory.
4.3.3 Relation to Historical Unification Programs
Previous unification attempts have generally followed one of two strategies:
Geometric extension (e.g., Kaluza–Klein theory)
Extending spacetime dimensionality to incorporate gauge fields geometrically [3,4].
High-energy symmetry unification (e.g., Yang–Mills, string theory)
Embedding interactions within larger symmetry groups or higher-dimensional frameworks [5–7].
Background-independent quantum gravity (e.g., loop quantum gravity)
Quantizing spacetime geometry itself [8].
MQ differs fundamentally from these approaches in that it does not begin with a continuum manifold. It does not introduce additional dimensions or symmetry groups ad hoc, and it does not quantize a pre-existing geometric structure. Instead, MQ constructs both geometry and gauge structure from a shared discrete kinematic origin. The unification is therefore foundational, occurring prior to both geometry and field-theoretic description.
This structural distinction has direct empirical implications. Because the MQ framework derives observable relations from count-dependent realization under the Frames mapping, it produces predictions that are, in principle, distinguishable from those of continuum-based formulations. These predictions satisfy a critical requirement emphasized in modern physics: that a theory must be empirically distinguishable from existing frameworks [43–46]. MQ is therefore not only structurally unifying, but also experimentally vulnerable – an essential property for scientific validity.
4.4 Conclusion
This work has established that a single count-based kinematic framework – formalized through the Frames mapping and governed by a unified action principle – can generate both electromagnetic and gravitational phenomena. The principal result is not merely that these domains can be described within a common formalism, but that they originate from the same underlying structure, without requiring separate foundational assumptions. In this sense, MQ provides a constructive resolution to the unification problem. It replaces the coexistence of distinct theoretical structures with a single generative mechanism.
At the same time, the scope of the present work remains appropriately bounded. While the emergence of gauge structure, metric behavior, and conservation laws has been demonstrated, a complete embedding into the full landscape of quantum field theory and gravitational phenomenology remains a subject of ongoing development.
The significance of MQ lies in three key contributions. It introduces a pre-geometric, count-based substrate underlying physical law. It demonstrates that action, symmetry, and geometry can emerge from this substrate. And it provides testable predictions that differentiate it from established theories. Taken together, these results position MQ not as a modification of existing theories, but as a candidate foundational framework from which they arise.
APPENDICES
APPENDIX A: DEFINITIONS OF KEYWORDS, TERMS AND SYMBOLS
Keywords
Internal Frame
The Internal Frame is the discrete, count-based configuration domain in which all fundamental measures are defined relative to the fundamental units lf, mf and tf. All relational structure is encoded as integer count configurations over this domain. The Internal Frame does not possess a continuous geometric structure; rather, geometry arises only through its mapping into the System Frame.
System Frame
The System Frame is the non-discrete, relational encoding of Internal Frame structure induced by the Frames mapping. It does not possess an independent fundamental measure but instead represents observable quantities as continuous relational separations derived from discrete count structure. All physically meaningful observables are defined in the System Frame.
Frames mapping
The Frames mapping is the kinematic transformation that relates discrete count configurations in the Internal Frame to continuous relational structure in the System Frame. This mapping preserves realization consistency and enforces closure conditions on relational configurations. Observable quantities arise only after application of the Frames mapping, and all geometric and interaction structure emerges from its properties.
Frames Principle
The Frames Principle asserts that all physically meaningful observables arise from the Frames mapping between the Internal Frame and the System Frame. No observable quantity is intrinsic to the Internal Frame alone. All measurement is relational and defined through the mapping. This principle replaces the assumption of a pre-existing spacetime manifold with a kinematic origin of geometry.
MQ Action
The MQ Action is the fundamental kinematic functional defined over the Internal Frame count structure. It governs the evolution and consistency of relational configurations under the Frames mapping. The action admits distinct realizations determined by count separation: fixed interaction-scale realizations, corresponding to electromagnetic behavior at the electromagnetic demarcation, and count-resolved realizations, corresponding to gravitational behavior through the mapping-induced metric structure. In both cases, observable dynamics arise from the normalization and realization of conserved count under the mapping. All emergent physical behavior, including electromagnetic interactions and gravitational curvature, therefore arises from this single action without the introduction of independent dynamical structures.
MQ variational principle
The MQ variational principle states that physically realized configurations in the System Frame correspond to stationary points of the MQ action functional defined over admissible realizations of encoded availability derived from the Internal Frame, thereby replacing the independent postulation of dynamical laws with a single extremization condition from which all effective interactions emerge. Formally, let M:ω→ℛ denote the Frames mapping, and let ω'⊂ω be a relational region of the Internal Frame with realized configuration Ω=M(ω')⊂ℛ. Let ρR denote the corresponding coarse-grained encoded availability field. The MQ action is defined as the functional
S[ρR]=∫Ωℒ(ρR,∂ρR,…) dμ,where ℒ is constructed from count-based relations induced by the mapping M, and dμ is the induced measure on ℛ. The MQ variational principle asserts that admissible realizations satisfy δS=0 under variations consistent with the constraints of the Frames mapping and the conservation relations defined on ω' (cf. Appx. E).
Informativity differential
The Informativity differential is the non-Lorentz length contraction associated with the discrete count structure of the Internal Frame. It arises from the normalization of conserved count under the Frames mapping and quantifies the difference between relational separation in the Internal Frame and its realized representation in the System Frame. The magnitude of the effect is count-dependent, increasing at small separations and diminishing toward the upper-count limit. The Informativity differential is distinct from curvature and represents one of the two geometric consequences of realization in the System Frame, the other being the emergent curvature associated with count loss under successive updates.
Metric differential
The metric differential characterizes the discrete–continuous mismatch that arises when conserved Internal Frame count structure is realized as a continuous observable in the System Frame under the Frames mapping. It does not represent a physical deformation in itself but rather the necessity of expressing integer-resolved count relations as normalized, non-discrete quantities.
For a fundamental measure defined by a count n in the Internal Frame, realization in the System Frame requires application of a mapping normalization functional. This process preserves count conservation while enforcing continuity, introducing a representation-level mismatch between the discrete count structure and its continuous encoding. The metric differential refers to this mismatch as a structural consequence of the mapping.
The metric differential is therefore distinct from the Informativity differential. While the Informativity differential describes a non-Lorentz length contraction in realized separations, the metric differential captures the underlying requirement that discrete count relations be expressed in a continuous form. In this sense, it provides the count-level representation of the discrete–continuous correspondence enforced by the Frames mapping, whereas the Informativity differential describes its realized geometric manifestation in the System Frame.
Electromagnetic demarcation
The electromagnetic demarcation is the fixed interaction count distance nL = 276/θsi, corresponding to approximately 84.60055lf, at which known electromagnetic interactions are realized in MQ. At this scale, the effect of the Informativity differential is still significant. Its influence increases with decreasing interaction distance and rapidly diminishes with increasing distance, becoming physically negligible beyond a few hundred counts of lf. The electromagnetic demarcation is the fixed electromagnetic interaction scale at which that discrete measure effect is realized.
Count separation
The number of fundamental length units lf between relational configurations in the Internal Frame. This quantity determines the scale at which mapping-induced deformation becomes significant.
Realization manifold
A realization manifold is the set of all admissible System Frame realizations compatible with a specified Internal Frame configuration under the Frames mapping ℛ(ΩI). The realization manifold is not a primitive geometric object of the Internal Frame. Rather, it is the image of conserved Internal Frame count structure after application of the Frames mapping and any applicable realization constraints. Probabilities are assigned only after a normalized measure is defined on the admissible realization manifold.
Mapping-induced deformation
The modification of realized separation in the System Frame arising from the discrete–continuous Frames mapping between the Internal Frame and the System Frame. This deformation is fully determined by the mapping structure and does not constitute an independent physical field. It has two coupled manifestations depending on the scale of the interaction. At fixed count separation, it appears as a local, scale-invariant modification governed by the Informativity differential, corresponding to the non-Lorentz contraction of realized lengths. Over extended count separation, the same mapping-induced deformation accumulates through the mapping structure and is realized as geometric curvature in the System Frame. These two manifestations are not distinct mechanisms but represent different scale-dependent realizations of a single underlying mapping effect.
Fixed interaction scale
A fixed interaction scale is a count-defined interaction distance at which a physical interaction is realized under the Frames mapping. For electromagnetic interactions, this occurs at the electromagnetic demarcation nL = 276/θsi, where the interaction is evaluated at a single, fixed count separation. At this scale, both the Informativity differential (non-Lorentz length contraction) and the corresponding curvature are realized with fixed values determined by the mapping. The interaction therefore reflects a specific point in the discrete count structure rather than a limiting description.
Curvature-resolved realization
Curvature-resolved realization refers to the dependence of realized geometric structure on count separation under the Frames mapping. In this description, curvature is a direct consequence of the mapping evaluated at a given count distance. Different separations correspond to different realized curvature values in the System Frame, providing a geometric description of interaction that varies with count scale. This behavior characterizes gravitational phenomena, where measurements probe a range of separations rather than a fixed interaction scale.
Terms
A.1 Primitive definitions
This subsection defines the irreducible count-based quantities that constitute the Internal Frame. These objects form the non-geometric substrate of MQ and serve as the primitive inputs to all subsequent constructions under the Frames mapping.
ℕ0 — the set of nonnegative integers {0,1,2, …}, used as the codomain for discrete count variables (e.g., nI, nS prior to density normalization).
ℤ — is the set of integers, used as the codomain for signed Internal Frame count-transfer quantities such as adjacency flux Jij. Positive and negative signs denote orientation of transfer along an admissible adjacency link and do not imply geometric direction in the System Frame.
ℝ3 — three–dimensional System Frame configuration space for single–subsystem spatial coordinates r.
ℝ3N — System Frame configuration space for an N–subsystem (or N–particle) encoded state Ψ(r1,…,rN,t).
A.2 Discrete Internal Frame primitives
This subsection establishes the primitive combinatorial and relational structures of the Internal Frame count substrate. These objects define admissible count configurations, adjacency relations, conservation structure, and regional count evolution prior to realization under the Frames mapping.
A — The Internal Frame update index is a discrete ordering parameter labeling successive configurations of the Internal Frame count medium. It indexes deterministic updates of relational count assignments nI(ξ,A) across the configuration domain ω, with regional evolution defined on subsets ω'⊂ω through conservation and adjacency relations. The update index A is not a physical time coordinate and carries no metric, geometric, or causal structure. It does not correspond to System Frame time t, nor to any observable temporal parameter. Instead, it provides an intrinsic ordering of count redistribution steps within the Internal Frame. Evolution with respect to A defines the deterministic conservation and redistribution of count via adjacency relations, as expressed in Internal Frame conservation laws of the form
= 0. The mapping between the Internal Frame update index A and System Frame time t is established only through the Frames mapping M, and is generally nontrivial. Consequently, A should be interpreted as a kinematic sequencing parameter intrinsic to the discrete count substrate, rather than as a temporal observable.
nI(ξ,A) — is the Internal Frame discrete measurement availability count at relational cell ξ and internal update index A; integer–valued with nI∈ℕ0. (No System Frame coordinates allowed.)
ρI(ξ,A) — is the Internal Frame count density at relational cell ξ and update index A. The quantity ρI represents the local distribution of measurement availability within the discrete relational structure of the Internal Frame. It is defined exclusively on the relational domain ω and carries no geometric, metric, coordinate, or continuum interpretation. The local count density ρI is constructed from the underlying count variable nI(ξ,A) and serves as the local conserved quantity appearing in Internal Frame conservation relations and adjacency–flux evolution equations. The evolution of ρI is governed by the discrete continuity relation
, or equivalently,
. The quantity ρI remains an Internal Frame object and must not be interpreted as a continuum mass density, probability density, or geometric field. Under the Frames mapping M, conservation of ρI provides the count structure from which realized System Frame observables and encoded availability measures are constructed.
NI(ω',A) — total Internal Frame count in a relational region Ω at internal update index A, typically
(or the appropriate internal measure analogue).
ξ — is a discrete relational cell label indexing elements of the Internal Frame configuration domain ω. Each ξ identifies a primitive micro-configuration at which Internal Frame count variables nI(ξ,A), density ρI(ξ,A), and adjacency flux JI(ξ→ξ',A) are defined. It may be described as ξ∈ω, ω'⊂ω, and
. The symbol ξ is a pure relational index and not a coordinate. It carries no metric, geometric, spatial, temporal, tangent-space, or continuum meaning. It is defined only through membership in ω, adjacency relations ξ∼ξ', and serves as a summation index and domain element for count density and flux. Under the Frames mapping, realizations derived from collections of relational cells contribute to emergent System Frame structures, but ξ itself never becomes a coordinate or vector in the realized continuum description.
ω — The Internal Frame configuration domain ω is an abstract relational domain containing all admissible Internal Frame count assignments and constraint systems on which candidate Frames mappings may be defined. It carries no metric, geometric, or temporal structure and does not correspond to any System Frame coordinate domain. A referenceable universe corresponds to a maximal subdomain U⊂ω on which a Frames mapping exists satisfying the global referenceability constraints (unique realization, normalization, and holonomy–free closure). Regional subsets ω'⊂ω are used to define finite count measures, conservation laws, and boundary–flux relations within the Internal Frame. The corresponding realized System Frame configurations are given by Ω=M(ω')⊂ℛ.
ω' — Is a relational region of the Internal Frame, with ω'⊂ω. This term denotes a finite subset of the Internal Frame relational adjacency domain used to define regional count measures, conservation laws, and boundary–flux relations. It carries no geometric or metric structure and does not correspond to a System Frame coordinate domain. Regional Internal Frame counts are written NI(ω',A).
∂ω — Adjacency boundary of an Internal Frame consisting of oriented adjacency links connecting cells in ω' to cells outside ω'. It appears in Internal Frame conservation relations through boundary–flux terms such as ϕI(∂ω',A).
Ω1,Ω2 — Internal Frame relational subsets used in finite additivity relations. They satisfy Ω1∩Ω2=∅ and NI(Ω1∪Ω2,A)=NI(Ω1,A)+NI(Ω2,A).
divadj — is the adjacency divergence operator acting on the Internal Frame count–flux JI. It is defined by
, where ∂Ω(ξ) denotes the set of admissible neighboring relational cells of ξ. The operator returns the net count imbalance associated with relational cell ξ during update step A by summing count–flux contributions over all admissible adjacency links incident on ξ. It is a purely combinatorial operator defined on the adjacency structure of the Internal Frame and carries no metric, geometric, directional, vector, or differential structure. The operator measures local count imbalance within the conserved count network and appears in the Internal Frame continuity relation
. It is a purely combinatorial operator defined on the adjacency structure of the Internal Frame and carries no metric, geometric, directional, vector, or differential structure. The operator measures local count imbalance within the conserved count network and appears in the Internal Frame continuity relation
. Equivalently,
. Unlike a continuum divergence, divadj does not act on a vector field and does not involve derivatives. It operates exclusively on count transfers between admissible neighboring relational cells. Under the Frames mapping, normalized realizations of the count–flux JI and adjacency divergence divadjJI correspond to the conserved current and its divergence in the System Frame, respectively.
Adj(ξ) — is the set of all relational cells ξ′ connected to ξ by an admissible adjacency link within the Internal Frame configuration domain ω. The adjacency neighborhood is a purely combinatorial object defined on the relational structure of the Internal Frame. It carries no metric, geometric, coordinate, vector, or continuum interpretation. Adj(ξ) specifies the relational cells that participate in local count redistribution through the adjacency count-flux JI(ξ → ξ′, A). It therefore provides the neighborhood structure used in the definitions of the adjacency divergence operator divadj, the local conservation law, and boundary-flux relations. Under the Frames mapping, realizations derived from Adj(ξ) may contribute to emergent System Frame structures, but Adj(ξ) itself remains an Internal Frame object and is not a geometric neighborhood in the System Frame.
JI — is the Internal Frame adjacency count–flux object defined on oriented adjacency links ξ→ξ' within the configuration domain ω. For each admissible link, JI(ξ→ξ',A) specifies the signed count transfer between relational cells during update step A. The object JI is the discrete flux structure associated with the conserved count field nI and provides the local transfer mechanism appearing in the Internal Frame continuity relation ΔAnI(ξ,A)+divadjJI(ξ,A)=0. JI is a purely combinatorial object defined exclusively on the adjacency structure of ω. It carries no metric, geometric, directional, vector, or differential structure. The relational cell labels ξ and ξ' denote adjacency relationships only and do not represent positions in a geometric space. Consequently, JI is not a vector field and no geometric differential operators act upon it. The associated adjacency divergence operator is defined by
, where N(ξ) denotes the set of admissible neighboring relational cells of ξ. This operator returns the net count imbalance associated with relational cell ξ during update step A and measures the local departure from count balance produced by adjacency transfers. Under the Frames mapping M, JI provides the discrete count-flux structure whose mapping-normalized realization defines the corresponding conserved current in the System Frame. The mapping does not reinterpret JI as a geometric vector. Rather, continuum current representations emerge through normalization of conserved count flow under the Frames mapping.
ϕI(∂ω' ,A) — is the Internal Frame boundary count–flux associated with a relational region ω' ⊂ω at update index A. It is defined as the net outward signed sum of adjacency flux contributions across all oriented boundary links connecting cells in ω' to cells in ω∖ω' ,
, where ∂ω' consists of all admissible oriented adjacency links with ξ∈ω' and ξ'∉ω' . This quantity represents the exact discrete boundary transport of measurement availability and has units of counts per update step. It is not a geometric surface integral and involves no notion of area, normal vectors, or metric structure. The boundary flux is related to the adjacency divergence of the count–flux through the discrete divergence relation, expressing regional conservation as the sum of local count imbalances over ω' . Under the Frames mapping, preservation of ϕI constrains the mapping normalization functional, thereby fixing how conserved Internal Frame flux is realized as a System Frame conserved current.
𝓁: an oriented adjacency link (edge) in the Internal Frame relational adjacency domain; elements of a closed loop γ are sequences of such links.
A.3 Frames Mapping and Realization Structures
This subsection defines the relational structures associated with admissible Frames mappings and referenceable universe domains. These objects govern normalization, realization, holonomy structure, record encoding, and the consistency conditions required for emergent System Frame observables.
U — is a referenceable universe domain when a maximal subdomain U⊂ω of the Internal Frame configuration domain on which a valid Frames mapping M exists satisfying normalization, unique realization, and holonomy–free closure on all contractible reference cycles. The corresponding System Frame reference structure is given by the relational image M(U)⊂ℛ. The domain U is maximal in the sense that no proper extension U'⊃U admits a Frames mapping satisfying the same global referenceability constraints. Distinct universes correspond to maximal subdomains whose associated Frames mappings cannot be simultaneously extended over their union without violating at least one global constraint.
γ — A reference cycle is a closed admissible relational path within a referenceable domain U⊂ω∖D used to evaluate loop functionals and consistency conditions associated with the Frames mapping. A reference cycle consists of a finite ordered sequence of admissible adjacency links returning to its origin. Contractible cycles must satisfy holonomy–free closure, while non–contractible cycles may carry defect-induced holonomy. Reference cycles are used to probe closure structure, measure consistency, and global referenceability conditions within admissible universe domains.
𝒞 — The count functional is a scalar functional acting on conserved Internal Frame count structure, mapping NI(ω',A) (and, where required, its associated density and flux structure) to a System Frame–compatible scalar prior to normalization. It encodes how relational count configurations contribute to realized observables independent of mapping normalization. More explicitly, it may be expressed as 𝒞:{ρI, JI, ∂ω'} → ℝ+, with the following constraints: i) consistency with conservation laws, ii) invariance under admissible Internal Frame relabelings, and iii) independence from System Frame coordinates.
f() — A System Frame observable function defined on the realized spatial coordinate domain ∈ℝ3. The function f() represents an arbitrary measurable quantity evaluated on a realized configuration and is used to construct expectation values over the normalized encoded availability density ρP(,t). It carries no primitive ontological status and does not correspond to an Internal Frame count variable, update index, or conservation quantity. Observable averages are obtained through expressions of the form
, or equivalently through the wave function encoding representation. The symbol fserves as a generic test function for realized System Frame observables and is not restricted to any particular physical quantity.
𝒩[ω' ]–The mapping normalization functional is a normalization operator induced by the Frames mapping that converts conserved Internal Frame count measures into System Frame observables by enforcing consistency with boundary–flux conservation and holonomy constraints. It acts on conserved count structure over a relational region ω'⊂ω and determines the normalization applied in the realization of M(ω'). Formally, it is given as
. Modified under discrete effects this is 𝒩[ω' ] → 𝒩[ω' ]⋅(2QLnLr).
ℒR[Ω] — Realized separation functional is a System Frame observable defined as a functional of conserved Internal Frame count structure over a relational region ω'⊂ω, obtained via the Frames mapping M. It assigns a measurable separation to a configuration of count density and adjacency relations without presupposing metric structure in the Internal Frame. The realized configuration is given by Ω=M(ω')⊂ℛ. Formally, it is described as ℒR[Ω] = ℱ(ρI(ξ,A), JI(ξ→ξ',A), ∂ω'), with realization ℒR[Ω] ≡ 𝒩[ω']⋅𝒞(NI(ω',A)) where 𝒩 is the normalization induced by mapping and 𝒞 is the count functional consistent with conservation laws.
ℛ — The System Frame realization structure ℛ is the relational image induced by the Frames mapping M:ω→ℛ, where ω is the Internal Frame relational domain. The structure ℛ comprises all admissible realized relational configurations consistent with the Frames mapping and the Frames Principle. It is not a pre-existing geometric manifold and does not constitute primitive ontology. Rather, it is the realized relational encoding through which observable System Frame quantities are represented. A realized physical system corresponds to a realized configuration Ω=M(ω')⊆ℛ, where ω'⊆ω is an admissible Internal Frame relational region. Realized coordinates, observables, realization manifolds, and encoded probability measures arise only within ℛ.
ℜ — is a realization manifold. ℜ⊆ℛ is the set of admissible System Frame realizations compatible with a specified Internal Frame configuration and any applicable realization constraints. Realization manifolds are induced by the Frames mapping and need not be unique. They may arise from constraints imposed by count separation, conservation laws, boundary conditions, contextual restrictions, or other admissible realization conditions. Probability measures are assigned only after normalization over the admissible realization manifold.
M — is the Frames mapping is a relational mapping M:ω→ℛ that assigns Internal Frame count configurations in the relational domain ωto elements of the uniquely realizable relational structure ℛdefining the emergent System Frame. A valid realization exists only on referenceable subdomains ω'⊆ω that satisfy normalization, repeatable realization, and holonomy-free closure on all contractible reference cycles. For any admissible subdomain ω', the corresponding realized configuration is Ω=M(ω')⊆ℛ. The mapping establishes consistent reference relations from which System Frame coordinates, observables, and realization structures are derived. Observable quantities arise only after application of the Frames mapping under the Frames Principle.
ℛξ∈ℛ — is a System Frame realization element ℛξ is an individual realized relational configuration associated with an admissible Internal Frame configuration ξ under the Frames mapping M. ℛξ∈ℛ. The collection {ℛξ} forms the realization structure ℛ. Realization elements encode relational information only and do not represent independent physical entities. Observable quantities arise from relations among realization elements within admissible realized configurations.
Ri — is the observer-specific macroscopic record state space associated with observer i. It consists of stable, observer-accessible realized states encoding measurement records and contextual outcomes. r∈Ri. Elements of Ri correspond to persistent realized record states that remain invariant under repeated observation and admissible evolution. Record states arise only after contextual restriction and normalization within the System Frame and therefore belong to the empirical layer of description rather than the primitive Internal Frame count structure.
E — is the admissible interaction set associated with a referenceable universe domain U. Elements x∈E denote admissible interaction configurations supporting realization under the Frames mapping. The set E is defined relationally within the Internal Frame and carries no continuum coordinate, metric, or geometric structure. Realization mappings assign outcome labels through R:E→O. The set E specifies the admissible interaction structure on which realization and record encodings are defined.
O — is the outcome label space associated with a referenceable Frames mapping. Elements o∈O are abstract realization labels assigned by the realization mapping R:E→O to admissible interactions x∈E. The set O is not a geometric or physical state space and carries no metric, coordinate, or dynamical structure. It indexes realizable outcomes within the System Frame encoding and serves as the domain of record encoding mappings ρ:O→ℛ. The realized outcome subset is OR:=R(E)⊆O, consisting of outcomes actually realized on a given admissible interaction structure.
τ — is a record relabeling bijection induced by an admissible outcome relabeling under a Frames automorphism. The map τ:ℛa→ℛb acts on realized macroscopic record states and preserves observable equivalence under relabeling of realized outcomes. For an outcome relabeling σ:OR→OR, the induced record relabeling satisfies τ(ρa(o))=ρb(σ(o)),o∈OR. The map τ preserves stable record distinguishability and introduces no change in geometric, closure, or measurable structure.
ρi:O→Ri — Record encoding mapping from outcome space O to macroscopic record states Ri. The mapping is injective on the realized outcome set OR, ensuring that distinct realized outcomes correspond to distinct observable records.
ℋ(γ) — A holonomy functional is the closure mismatch obtained by transporting reference data around a closed reference cycle γunder the Frames mapping. For holonomy–free mappings, ℋ(γ)=0 on all contractible cycles.
D — A mapping defect class is a global obstruction in the Frames mapping preventing extension of a holonomy–free mapping across the full configuration domain. Persistent defects anchor universe initiation and determine the holonomy class of the resulting reference structure.
Φ — A frames automorphism is an invertible transformation Φ:U→U acting on a referenceable universe domain U⊂ω that preserves the structural constraints of the Frames mapping M, including normalization, repeatable realization, and holonomy–free closure on contractible cycles. Two universe realizations related by Φ are physically equivalent descriptions of the same System Frame structure.
𝒞s — is the set of admissible Internal Frame configurations that correspond to a single System Frame state s under a valid Frames mapping. It represents the pre-image of s and defines the domain over which encoded availability weights are assigned and normalized.
A.4 Emergent System Frame Continuum Structures
This subsection establishes the continuum relational structures induced through the Frames mapping. These objects define encoded availability densities, emergent coordinate representations, continuum observables, and associated differential structures within the realized System Frame.
Ω — It denotes the System Frame image of a relational region ω'⊂ω under the Frames mapping M, such that Ω=M(ω'). The set Ω consists of encoded relational configurations corresponding to physically realized systems and carries the continuous relational structure in which observables are defined. It is not an Internal Frame domain and does not support count–based conservation laws directly.
𝒜 — System Frame log–gradient availability potential. Vector field defined on the System Frame continuum encoding by 𝒜 ≡ ∇lnρR, where ρR is the System Frame encoded availability density. This field measures the fractional spatial variation of encoded availability and represents the natural connection structure associated with multiplicative rescaling of ρR. It emerges from the Frames mapping of the Internal Frame count measure and has no counterpart in the Internal Frame. Under a multiplicative rescaling of encoded availability,
, the field transforms as 𝒜 → 𝒜'=𝒜+∇χ, establishing its role as an emergent Abelian gauge potential in the System Frame representation.
nk(t)— encoded availability in partition Ak
. Represents the pre–normalized encoded availability in region Ak. Used to construct conditional probabilities via normalization: P(k)=nk(t)/N1(t).
ρS(,t) — System Frame encoded availability density
.
Continuum density obtained from the deterministic Frames mapping applied to the Internal Frame count measure. It is the Radon–Nikodym derivative of the induced System Frame count measure with respect to Lebesgue volume. Non–negative and integrable over finite regions. The total encoded availability is N1(t)=∫ρS(,t) d3. Not normalized in general. Represents encoded measurement availability prior to probabilistic interpretation. Serves as the fundamental System Frame scalar from which ρpand all observable statistics are derived.
nS(,t) — discretized System Frame availability count field. Discrete encoded availability count associated with a System Frame cell (index j) or region A at time t, obtained via the Frames mapping from Internal Frame availability. Integer–valued when discretized. Used for counts and partitions (e.g., nS,j(t) or nS(A,t)), not as the argument of continuum differential operators.
AS(,t) — System Frame log–gradient availability field (dimension 1/length), defined by
measures fractional spatial variation of encoded availability density.
— is the System Frame spatial coordinate vector ∈ℝ3 of the realized System Frame continuum. Used to parameterize encoded availability densities, probability densities, currents, velocity fields, wavefunctions, and other nonrelativistic observables arising from the Frames mapping. Appears in expressions such as ρS(,t), P(,t), J(,t), (,t), Q(,t), and ψ(,t). Represents position within the realized three-dimensional spatial domain Ω. Distinct from the spacetime coordinate μ used in relativistic and geometric formulations.
Vμ(x) — is a smooth contravariant vector field defined on the emergent System Frame continuum. It is used to represent tangent vectors, transport directions, currents, variational displacements, and other geometric quantities arising after application of the Frames mapping. The field carries standard continuum geometric meaning with respect to the emergent metric
and is acted upon by covariant derivatives, connections, and curvature operators. Unlike the Internal Frame relational cell label ξ, the quantity Vμ is not a count index and possesses no direct interpretation within the discrete count substrate. It exists only in the realized continuum description induced by the Frames mapping. Generic continuum identities such as
are therefore statements about emergent System Frame geometry rather than primitive Internal Frame count structure.
xμ — is the System Frame spacetime coordinate xμ=(x0,x1,x2,x3). Four-dimensional coordinate on the emergent System Frame spacetime manifold. Used in continuum geometric constructions including the metric tensor
, connection coefficients
, curvature tensors, geodesics, action functionals, and covariant field equations. Coordinates are defined on the realized manifold induced by the Frames mapping. The spatial components of xμ reduce locally to the realized spatial coordinates represented by , but xμ is reserved for relativistic and differential geometric formulations.
t — System Frame time coordinate used in the continuum encoding and Schrödinger evolution.
rA,rB — System Frame spatial coordinate vectors for subsystems A and B in a bipartite (entanglement/Bell) configuration.
A.5 Realized separation and metric structure
This subsection introduces the realized separation functional and its continuum encoding in the System Frame. The emergent metric is defined as the tensor that reproduces the mapped separation relations under coarse-graining of the discrete count structure.
N1(t) — total encoded availability count in the single–subsystem System Frame normalization, defined by the inline equation
.
N2(t) — total encoded availability count in the bipartite (two–subsystem) System Frame normalization, defined by the inline equation
.
ρP(,t) — normalized System Frame probability density
. Dimensionless normalized probability density derived from the realized encoded availability density ρS(,t). Defines realized outcome probabilities and detection statistics within the System Frame. The MQ wave function satisfies
. Probability in MQ arises exclusively from normalization of realized encoded availability ρS, not from primitive Internal Frame randomness. All probabilistic and field-theoretic constructions in the System Frame are defined with respect to ρP.
ρP1(,t),ρP2(,t) — marginal System Frame probability densities for subsystems 1 and 2 obtained by integrating the joint realized probability density over the complementary subsystem coordinates.
𝒪out — The System Frame output domain Oout⊂ℛ is the realized relational region associated with measurement readout, whose measurable partition {Ak} defines distinct macroscopic record classes. These subsets satisfy ⋃kAk=Ooutand Ai∩Aj=∅for i≠j. The domain Oout exists only in the System Frame as a partitioned subset of the realized relational structure and has no counterpart in the Internal Frame. Probabilities associated with outcomes are obtained by normalization of encoded availability over the partition elements Ak, and distinct subsets correspond, via the record encoding mapping, to distinct macroscopic record states.
Ak — is subset Ak⊂Oout⊂ℛ is a measurable region of the System Frame output domain corresponding to a distinct macroscopic record class or measurement outcome channel. The collection {Ak} forms a mutually exclusive and exhaustive partition satisfying Ai∩Aj=∅ for i≠j and ⋃kAk=Oout. Probabilities are obtained by normalization of encoded availability over these subsets, with outcome weights given by
, where ρ is the System Frame encoded availability density. The subsets Akexist only within the realized System Frame encoding and have no counterpart in the Internal Frame. Distinct subsets correspond, via the record encoding mapping, to distinct macroscopic record states. Indicator functions associated with Ak define restriction and conditioning operations within the encoded Hilbert space representation.
— is associated with each subset Akis the indicator function
, defined by
for ∈Ak and 0 otherwise, which implements restriction and conditioning of encoded availability and wave function support to the corresponding measurement region.
ψ(,t) — is the encoded System Frame wave function in the position representation; ψ∈L2(ℝ3). The wave function provides the position space representation of the encoded System Frame state ∣Ψ⟩ and may be expressed in Madelung form as
∣Ψ⟩ — is the encoded System Frame state vector in Hilbert space; used for basis expansions, projection updates, and expectation values.
A.6 Differential and operator structure
This subsection defines the operators acting on realized quantities in the System Frame. These include mapping-consistent derivative and update structures that enable the construction of curvature and field equations from the emergent metric.
∇ — System Frame gradient operator acting on continuum–encoded fields.
∇⋅ — System Frame divergence operator acting on geometric vector fields.
H — System Frame Hamiltonian operator governing unitary Schrödinger evolution (in the encoded continuum representation), typically H=-ħ2/(2m)∇2+V(,t).
— System Frame Hamiltonian operator governing unitary Schrödinger evolution in the encoded continuum representation. For a non-relativistic encoded state,
. The operator
is the continuum realization of the admissible discrete redistribution generator Hd obtained under the Frames mapping. It acts on encoded System Frame wave functions Ψ(,t) and generates Schrödinger-form evolution through
. The operator represents redistribution dynamics of normalized encoded availability under closed evolution. Under the admissibility and boundary conditions,
is Hermitian and generates unitary evolution of the encoded state.
U(t) — unitary time–evolution operator in the System Frame Hilbert representation: U(t)=e-iHt/ℏ.
V(,t) — potential energy function in the System Frame Schrödinger equation; may include external fields and interactions as encoded in the continuum representation.
ϕ(,t) — is the dimensionless System Frame phase field of the encoded wave function ψ(,t). The phase determines interference structure and generates momentum and velocity fields through its spatial and temporal gradients.
S(,t) — is the phase action field of the encoded wave function. S(,t) carries units of action and is related to the dimensionless phase field by S(,t)=ħ ϕ(,t).
(,t) — is the System Frame velocity field in Madelung form, (,t)=(ℏ/m)∇ϕ(,t)=(1/m)∇S(,t).
(,t) — momentum field in the System Frame phase gradient representation, (,t)=ℏ∇ϕ(,t)=∇S(,t), with =m v when a velocity field is defined.
— momentum operator in position representation:
.
𝑺𝑻ρ(,t) — System Frame probability current density defined with respect to the normalized density ρp. It satisfies the continuity equation ∂tρp+∇⋅𝑺𝑻ρ=0. In Madelung form,
Represents conserved probability flow in the System Frame. This current is not defined for ρS, ensuring consistency between conservation laws and normalized observables.
Δd — Discrete Laplacian (difference–operator Laplacian) defined on the lattice/adjacency structure of the Internal Frame. It is the discrete analog of the continuum operator ∇2, constructed from adjacency relations ξ∼ξ' and acting on count–defined fields. In the continuum limit, it approximates the standard Laplacian via
. This operator is used in the lattice/adjacency discretization of dynamical equations, including Schrödinger–type evolution, and encodes second–order relational variation across adjacent Internal Frame configurations.
Hd — discrete Hamiltonian operator used in lattice/discretized dynamics, typically Hd=-ħ2/(2m) Δd/(Δx)2+V, with Δd the discrete Laplacian defined on the chosen adjacency/lattice and Δx the spatial step.
Q(,t) — quantum potential (Madelung form)
Defined strictly in terms of the normalized density ρp. Encodes quantum corrections to the Hamilton–Jacobi–like equation arising from the encoded availability structure after normalization.
A.7 Fundamental constant and measures
This subsection collects the invariant constants and normalization measures that appear in the MQ framework. These quantities fix the scale of mapping between discrete counts and continuum observables without introducing independent phenomenological parameters.
lf,mf,tf — are the fundamental measures, more precise expressions for Planck’s units–length, mass, and time–that consider the effects of length contraction associated with discrete measure.
2QLnLr — also known as the Informativity differential describes the length contraction associated with discrete measure. It is a dimensionless normalization modifier arising from the discrete count structure of the Internal Frame, representing the deviation between integer–resolved count measures and their realized System Frame encoding under the Frames mapping M:ω→ℛ. It quantifies how conserved Internal Frame count NI(ω',A) is redistributed and normalized when expressed as a System Frame observable.
G — is the gravitational constant, G=6.67407794(17) × 10–11 m3 kg–1 s–2 [47] such that its value considers the effects of length contraction associated with discrete measure at the upper count limit. Italicized G identifies a measure (e.g., G=6.67384483(17) × 10–11 m3 kg–1 s–2 [48] at the blackbody demarcation ([9], Appx. AB)).
θsi — can be measured as the polarization angle of quantum entangled X–rays at the degenerate frequency of a maximal Bell state. As an angle θsi=3.26239 rad ± 2 μrad [49]. As a momentum θsi = 3.262390305(89) kg m s–1. And with respect to the System Frame, θsi has no units.
c is the speed of light which may also be written as c=nLlf/nTtf =299,792,458 m/s [50] such that nL=nT=1 is physically significant.
H0 describes the rate of expanding space between galaxies. MQ expands this nomenclature as a function of two parameters. Expansion can be described either as a function of the local rate H (km s–1 Mpc–1) or the scalar rate H (i.e. magnitude). Terms describe either observed expansion (subscript 0) or metric expansion (no subscript).
HCMB describes the rate of expansion in km s–1 Mpc–1 as resolved using CMB data, also known as the Hubble constant H0.
Hcep describes the rate of expansion between galaxies in km s–1 Mpc–1 as resolved using cepheid data, also known as the Hubble constant H0.
Hsys represents a System Frame description of the Hubble constant as would be consistent with a CMB study. This calculation describes the metric expansion of space relative to the non–discrete System Frame.
Hint represents an Internal Frame description of the Hubble constant as would be consistent with a cepheid study. This calculation describes the metric expansion of space relative to the discrete Internal Frame.
Hb represents the baseline expression which falls at the midpoint of Hsys and Hint.
H describes the scalar rate of expansion associated with the increasing radius of the universe. For our universe, this non–dimensional scalar is described by, H=θsi.
H0 describes the observed scalar rate of expansion associated with the increasing radius of the universe. There is no measure of this value at this time.
lp, mp and tp are Planck’s units for length, mass, and time.
nL, nM and nT are physically significant discrete counts of lf, mf and tf respectively.
nL describes the count of lf representative of a change in position of an observable measured with respect to the observer’s frame of reference.
nTu is a count of tf equal to the age of the universe.
nLu is a count of lf equal to the diameter of the universe.
nLc describes the count of lf representative of a change in position of light measured with respect to the observer’s frame of reference.
nθ is the System Frame count of θsi resolved as a function of the Internal Frame demarcation adjusted for the metric differential (i.e., ⌊84.60055/2⌉ = 42).
h is Planck’s constant.
ℏ is the reduced Planck constant, 1.054571817 10–34 m2 kg s–1. When accounting for the Informativity differential at the upper count bound, this term is not italicized (i.e., ħ=1.054534984(26) 10–34 m2 kg s–1).
Aee is the dilated age of the universe as measured from the current expansionary epoch. Its value is a function of expansion with respect to the total elapsed time representing the quantum epoch.
Aqe is the non–dilated age of the universe corresponding to the quantum epoch.
Vqe describes the volume of the universe at the end of the quantum epoch.
Ωvis is that domain of the universe that is presently visible.
Ωobs is that domain of the universe that is presently visible or will be visible given infinite elapsed time.
Ωdk is that domain of the universe that will never be visible.
Ωuobs is that domain of the universe that will eventually be visible but is not presently visible.
Ωtot is the entire domain that makes up the universe (i.e., 1 or 100%).
Ωf is that domain of the universe that is fundamental. Its physical significance describes a pivot point with respect to the remaining domains.
Mtot is the total mass of the universe, including all forms of energy.
Macr is the rate of mass accretion in the universe.
me is the mass of an electron.
a0 is the ground state orbital of an atom, also known as the Bohr radius.
αf–1, αp–1, and αc–1 are the fundamental, Planck–like, and classical forms of the inverse fine structure constant. αf–1=42θsi is defined with respect to the System Frame; the remaining two against the Internal Frame such that αc–1 differs from αp–1, accounting for the length contraction associated with discrete measure.
γ is a collection of terms that describe the geometry between the System and Internal frames.
Λ describes Einstein’s cosmological constant.
ɛ0 is the electric constant.
u0 is the magnetic constant.
ke is Coulomb’s constant.
e— is elementary charge.
ECMB is the total energy associated with the CMB.
Eρ:cmb is the energy density associated with the CMB.
k is the Boltzmann constant.
ρ is the energy density accumulated at a given age of the universe.
TCMB is the temperature of the Cosmic Microwave Background.
A.8 Expansion and cosmological scalars
This subsection defines the scalar quantities governing expansion in MQ, including mapping-derived normalization factors and cosmological terms. These quantities describe the homogeneous expansion as it emerges from count-based structure under the Frames mapping.
t — denotes the global ordering parameter labeling the one-parameter family of realized configurations in the System Frame. It provides the monotonic parameterization of expansion as defined by the evolution of the mapping-realized separation functional and does not represent a primitive temporal coordinate in the Internal Frame.
a(t) — denotes a derived System Frame scale function used to parameterize the evolution of realized separations under mapping normalization. It is strictly increasing and piecewise differentiable but does not constitute a fundamental degree of freedom; rather, it provides a convenient parametrization of expansion extracted from the underlying separation functional.
l — denotes an invariant internal reference scale associated with the mapping-normalized separation structure. It remains constant under expansion and serves to fix the reference normalization relating discrete count structure to realized System Frame separations, without introducing an independent dynamical scale.
QL — denotes the mapping-induced residual count contribution entering the realized separation functional. In the right-triangle count construction, nL gives the Internal Frame count separation, while nL + QL gives the realized hypotenuse whose continuum encoding defines the System Frame separation. QL therefore replaces the older Internal-to-System scale-ratio notation by expressing expansion and curvature through count-resolved residual structure rather than through a global ratio.
ΛMQ — denotes the MQ-derived cosmological term obtained from the scalar contribution after mapping-consistent normalization. It is not introduced phenomenologically in the action but is fixed by the expansion structure and realized separation relations used to construct the metric and field equation.
Λsys — denotes the System Frame realization of the MQ cosmological term, evaluated using the System Frame expansion rate. It represents the continuum-frame scalar contribution entering comparison with CMB-inferred cosmological determinations.
Λint — denotes the Internal Frame realization of the MQ cosmological term, evaluated using the Internal Frame expansion rate. It represents the discrete-frame scalar realization associated with the corresponding mapping-normalized expansion structure.
A.9 Mapping and normalization symbols
This subsection collects symbols associated with mapping normalization and the single-action realization of dynamical quantities under the Frames mapping. It includes the functions and parameters that convert dimensionless scalar quantities into their observable, unit-resolved forms and govern admissible dynamical variation.
ρf— denotes an invariant, dimensionless internal geometric normalization factor used in the mapping of homogeneous expansion. It is not the FRW scale factor and does not define the general emergent metric. Its role is limited to fixing the reference normalization through which discrete count evolution is related to continuum expansion in the homogeneous limit.
ΔH — denotes the mapping-induced normalization offset between System Frame and Internal Frame realizations of the scalar expansion parameter. It is defined by ΔH=θsi-π and represents a frame-resolution offset under the Frames mapping, not an independent dynamical parameter or a global count-expansion mismatch.
H— denotes the dimensionless scalar rate of radial expansion defined at the level of the System Frame realization of the Frames mapping. It represents the intrinsic expansion magnitude governing the growth of realized separations and is independent of observational units. Within MQ, H = θsi, so that H is not a measured local rate but the mapping-defined scalar controlling the expansion geometry and associated mapping-consistent scalar relations.
H0— denotes the dimensionful expansion rate expressed in observational units (e.g., km s-1
Mpc-1). It is obtained through mapping-consistent normalization of the scalar H, converting the dimensionless expansion into a measurable quantity. It does not constitute an independent parameter, but rather the observational representation of H under a specified measurement convention at the present epoch.
Hsys— is the System Frame realization of the expansion rate, obtained by expressing the scalar H under mapping normalization consistent with the non-discrete relational encoding. It corresponds to expansion values inferred from CMB-based measurements and represents the continuum realization of the underlying scalar expansion.
Hint— is the Internal Frame realization of the expansion rate, obtained by expressing the scalar H under mapping normalization consistent with discrete count structure. It corresponds to expansion values inferred from local distance-ladder measurements and differs from Hsys by a mapping-induced normalization offset rather than by an independent physical parameter.
H — denotes the dimensionful local expansion rate expressed in observational units (e.g., km s-1 Mpc-1), prior to specification of a particular frame realization. It represents the normalized, unit-resolved form of the scalar expansion parameter H and serves as the general observable expansion rate from which specific realizations such as H0, Hsys, and Hint are defined.
S — denotes the single MQ action functional defined over the count structure and its coarse-grained realization under the Frames mapping. It supplies the common variational origin of the metric, curvature, source, coupling, and scalar contributions, so no independent gravitational or matter action is fundamental at the primitive level.
Sg— denotes the geometric contribution to the realized action when the single MQ action is expressed in continuum form. It is a derived representation of the curvature constructed from the emergent metric, not an independently postulated Einstein-Hilbert action.
Sm— denotes the matter contribution to the realized action when the single MQ action is expressed in continuum form. It defines the stress-energy tensor through variation with respect to the emergent System Frame metric and is not an independently specified matter description. The paper states that the stress-energy tensor is obtained by varying the same action with respect to the emergent metric.
ℒ— denotes the realized Lagrangian density appearing in the MQ action. It is constructed from mapping-induced quantities and contains no independent gravitational coupling or separate primitive decomposition.
ℒm— denotes the matter Lagrangian density in the realized continuum representation. It is constructed from encoded availability, its derivatives, and the emergent metric, with admissible terms fixed by the MQ variational principle rather than by an independently postulated matter description.
A.10 Field equation components
This subsection defines the geometric and source terms entering the MQ field equation. These quantities are constructed from the emergent metric and mapping-consistent action, ensuring that curvature, stress-energy, and coupling arise from a single unified framework.
ρtot— the total density
inferred from the MQ System Frame expansion rate corresponds to the observationally inferred cosmic energy density when the MQ kinematic expansion law is interpreted within the standard gravitational framework.
ρc— the critical density ρc=3H2/8πG is the total energy density required for spatial flatness in the standard Friedmann–Lemaître cosmological model. It provides the conventional normalization scale against which fractional density components are defined.
ρΛ— the vacuum density ρΛ=Λ c2/8πG is the effective energy density associated with the cosmological constant term appearing in Einstein’s field equations. In the MQ framework, this quantity corresponds to the dynamical realization, within general relativity, of the geometric scalar derived from invariant measure relations.
ρm— the matter density ρm=(1-ΩΛ)ρc represents the non–scalar contribution to the total cosmic energy density. Under the assumption of spatial flatness, it corresponds to the complement of the scalar fraction and includes both baryonic and dark matter components.
ρMQ— the MQ geometric density
is the density scale arising directly from invariant fundamental measure normalization in the Internal Frame. It depends only on the geometric scalar Λand the fundamental length measure lf, and does not involve the gravitational coupling constant. This quantity represents the kinematic density associated with the induced scalar prior to any dynamical interpretation.
ΩΛ— The fractional scalar density parameter ΩΛ=ρΛ/ρc=Λ c2/3H2 specifies the proportion of the total cosmic energy density attributed to the scalar contribution. Within MQ it is determined entirely by invariant internal relations.
Ωb— baryonic matter fraction (ΛCDM comparison bookkeeping).
Ωc— cold dark matter fraction (ΛCDM comparison bookkeeping).
gμν — The quantity gμν denotes the emergent metric tensor in the System Frame. In standard general relativity, gμν is a fundamental field defining spacetime geometry. In MQ, it is a derived object obtained through coarse–graining of the realized separation functional induced by the Frames mapping. Its normalization is fixed by mapping constraints and not freely specified.
Gμν— The tensor Gμν is the curvature tensor constructed from gμν through second–order differential structure. In MQ, it represents the continuum limit of the discrete second–difference operator acting on count displacement in the Internal Frame. Its divergence–free property follows from mapping–induced invariance, not from an independent geometric postulate.
Tμν — The tensor Tμν denotes the stress–energy tensor in the System Frame. In MQ, it is defined variationally from the matter contribution to the MQ action,
and therefore encodes the response of normalized count density to variations in the emergent metric. It is not independently specified and inherits its structure from encoded availability and mapping normalization.
Λ — The scalar Λdenotes the cosmological term appearing in the continuum field equation. In MQ, it is not a fundamental constant but a derived scalar arising from the same realized separation structure that defines the emergent metric
. It reflects the large-scale normalization of the System Frame geometry induced by the Frames mapping and is therefore fixed by the underlying count geometry, not introduced as an independent parameter.
APPENDIX B: MQ KINEMATICS AND THE ACTION PRINCIPLE
This appendix consolidates the kinematic construction and action formulation underlying the Frames mapping and the single action principle, expressed strictly in terms of established MQ primitives and previously defined quantities.
B.1 Internal–System Frame Kinematic Structure
Let the Internal Frame configuration domain be defined as a countable relational set ω, where ω carries no intrinsic metric, geometry, temporal duration, or continuum coordinate structure. The Internal Frame is ordered by the update index A, which labels successive configurations of the count substrate but does not correspond to a physical time coordinate. Each relational cell ξ∈ω carries a discrete measurement availability count nI(ξ,A), representing measurement availability within the Internal Frame. For a relational region ω'⊂ω, the total regional count is defined as
consistent with Eq. (71) of the main text.
Local evolution of measurement availability is governed by the Internal Frame continuity relation
which expresses conservation through redistribution of count across admissible adjacency links. Here JI denotes the Internal Frame adjacency count-flux object, while (divadjJI)(ξ,A) measures the net count imbalance associated with relational cell ξarising from admissible adjacency transfers. No geometric, coordinate, vector, or continuum structure is assumed.
Summing Eq. (B.2) over a finite relational region ω' yields the regional conservation relation
where the boundary count-flux is defined by
The quantity ϕI(∂ω',A) represents the exact net outward transport of measurement availability across the adjacency boundary ∂ω'. It is a discrete count-flux defined entirely on the relational adjacency structure of the Internal Frame. It is not a geometric surface integral and carries no dependence on area, normal vectors, metric structure, or continuum geometry.
These conservation relations are purely combinatorial statements defined on the relational structure of the Internal Frame. The quantities nI, NI, JI, and ϕI are count-based objects defined exclusively on the relational domain ω, while divadjis a combinatorial operator acting on admissible adjacency transfers. Length, distance, volume, coordinates, and all observable geometric quantities arise only through admissible realization under the Frames mapping M:ω→ℛ, which assigns Internal Frame count configurations to elements of the realized System Frame relational structure ℛ.
Under the Frames mapping, conserved Internal Frame count induces a realized encoded availability measure on the corresponding System Frame configuration. When this induced measure is absolutely continuous with respect to the realized System Frame volume element d3r, the encoded availability density is defined as the Radon–Nikodym derivative
where NI denotes the conserved Internal Frame count measure realized through the mapping. The coordinates and t are System Frame quantities and arise only after realization under M. Consequently, ρS is not a primitive Internal Frame object. Rather, it is the mapping-normalized realization of conserved count within the emergent System Frame representation.
The total realized encoded availability over the relevant System Frame region Ω is therefore
and normalization yields the System Frame probability density
In this formulation, all System Frame observables are normalized representations of conserved Internal Frame count structure. The hierarchy ρI→ρS→ρP corresponds respectively to the discrete count density, the realized encoded availability density induced by the Frames mapping, and the normalized probability density obtained from that realization. In conventional quantum mechanical notation, the probability density is often denoted by P(,t). Within MQ, we retain the notation ρP(,t) to preserve the explicit relationship between count density, encoded availability, and probability. Thus, P(,t)≡ρP(,t), but the latter notation makes the origin of the probabilistic description in conserved Internal Frame count structure explicit. The Frames mapping M therefore provides the bridge between discrete count structure and continuum physical observables without introducing continuum geometry into the primitive Internal Frame.
B.2 Log gradient Field and Kinematic Encoding
Define the System Frame log gradient availability field
where ρ(,t) is the realized availability density as introduced. The operator ∇ is the System Frame gradient and is defined only after realization through the Frames mapping M:ω→ℛ. This field encodes the spatial variation of the normalized count measure and therefore captures all admissible kinematic variation arising from the underlying Internal Frame count structure under the Frames Principle. Because ρP is a normalized representation of conserved count, the log gradient isolates relative variation independent of absolute normalization.
The corresponding current density is defined as
where P(x,t)=ρ(,t)/N is the normalized probability density.
The velocity field is introduced as a potential flow generated by a scalar field S(,t),
where S(,t) is a System Frame scalar potential associated with the realized kinematic state. In this formulation, S plays the role of a generating function for admissible flow consistent with the mapped count structure. The introduction of S does not constitute an independent dynamical assumption. Rather, it provides a minimal representation of admissible velocity fields consistent with the log gradient encoding and the conservation structure established in Sec. B.1. The resulting current 𝑺𝑻(,t) therefore reflects the transport of normalized count density under the realized mapping.
B.3 MQ Action Functional
The MQ action is defined over the System Frame encoding induced by the Frames mapping M:ω→ℛ. Let 𝒮 denote the action functional, distinct from the scalar field S(,t) introduced in Sec. B.2. The action is given by
where:
S(,t) is the System Frame scalar field generating the velocity field via
, as introduced in Sec. B.2.
V(,t) is the System Frame potential associated with external or emergent interaction structure.
ρP(,t) is the realized availability density obtained from the mapped Internal Frame count measure (Sec. B.1). It is not an independent field, but a normalized representation of conserved count structure.
∂t denotes differentiation with respect to System Frame time t, which arises only after realization through the Frames mapping.
The term Q(,t) is given
and represents the MQ quantum potential. In the present framework, this term is not introduced as an independent dynamical assumption but arises from the continuum encoding of discrete count geometry under the mapping and normalization constraints.
The action 𝒮 provides a unified dynamical description of admissible System Frame configurations. Stationarity of the action under variations of ρP(,t) and S(,t) yields the governing evolution equations for the encoded fields, consistent with the conservation structure established in Sec. B.1 and the kinematic encoding introduced in Sec. B.2.
B.4 Variational Principle
Admissible variations of the action 𝒮 are taken with respect to the fields ρ(,t) and S(,t), subject to the normalization constraint
where NI denotes the conserved Internal Frame count realized in the System Frame representation under the Frames mapping (Sec. B.1). Variations δρ are therefore constrained to preserve this normalization. The fields are assumed sufficiently smooth for the variational procedure to be well-defined within the System Frame representation.
Variation of the action (Eq. B.11) with respect to S(,t) yields
which is the continuity equation. In the MQ framework, this equation is not postulated but arises as the System Frame expression of conserved Internal Frame count under the mapping M:ω→ℛ. Variation with respect to ρP(,t) yields
which has the form of a Hamilton–Jacobi equation. Here, it represents the kinematic constraint governing admissible realizations of the mapped count structure rather than an independent dynamical assumption.
The velocity field v(x,t), defined by
is therefore determined consistently with both conservation and the variational structure of the action.
Taken together, Eqs. (B.14–B.15) provide a closed System Frame representation of the evolution of realized observables. Their origin in the MQ framework lies entirely in the conservation and normalization of count structure under admissible mappings, rather than in postulated continuum dynamics.
B.5 Schrödinger Representation
Define the MQ wavefunction as a complex encoding of the realized count structure,
where P(,t)=ρ(,t)/NI is the normalized availability density and S(,t) is the System Frame scalar field introduced in Sec. B.2. The field ψ(,t) is not a fundamental object, but a derived representation that combines amplitude (count density) and phase (kinematic encoding) into a single complex field.
In this representation, the continuity equation (Eq. B.14) and the Hamilton–Jacobi form (Eq. B.15) obtained from the MQ action combine into a single complex evolution equation. Combining these equations yields
which is the Schrödinger equation.
Within the MQ framework, this equation is not postulated. It arises as a compact representation of two underlying structural relations: conservation of Internal Frame count under the Frames mapping M:ω→ℛ, and the kinematic constraint governing admissible realizations of that count structure. The quantum potential Q appearing in Eq. (B.13) is absorbed into the complex phase representation, eliminating the need to treat it as a separate dynamical term.
The constant ħ enters as the scale relating the phase field S to the complex representation. In MQ, this scaling reflects the discrete–continuous correspondence between Internal Frame count geometry and its System Frame encoding, rather than an independent postulate.
Thus, the Schrödinger equation emerges as a derived consequence of count-based kinematics. Standard quantum dynamics is recovered as the minimal complex representation of conserved and admissibly mapped count structure.
B.6 Action Consistency with Discrete Measure
The MQ action (Eq. B.9) is constrained by the discrete–continuous mapping of Internal Frame count structure into System Frame observables. This mapping introduces the Informativity differential, expressed as
which governs the asymptotic recovery of continuum behavior. For finite count separation nL, the factor 2QLnL modifies the effective realization of spatial measures. This modification does not alter the underlying count structure but instead deforms the System Frame representation of length entering all dynamical terms. As a result, the quantities appearing in the action – specifically the kinetic term (∇S)2, the potential V(,t), and the quantum potential Q(x,t) – are implicitly functions of the count-dependent realization of separation. Accordingly, the action is more precisely understood as
where the dependence on nL enters through the mapping-induced deformation of spatial measures rather than through explicit dependence on raw counts. Note the difference between script ‘S’ and italic ‘S’. Script S denotes the action functional, distinct from the scalar field S(x,t).
A central consequence is that different interaction channels probe different effective realizations of length. Electromagnetic interactions occur at the fixed electromagnetic demarcation (i.e., nL = 276/θsi for charge couplings), while gravitational interactions are resolved at count scales determined by the macroscopic separation of the system. Because the Informativity differential depends on nL, the effective normalization of realized observables differs between these interaction channels.
This leads directly to a physically testable prediction: quantities inferred through electromagnetic interactions incorporate a systematic correction arising from discrete length contraction, while quantities inferred through gravitational interactions approach the continuum limit where 2QLnL → 1. The action therefore encodes not only the dynamical evolution of observables, but also the interaction-dependent realization of those observables through the Frames mapping.
In this sense, the MQ action is consistent with discrete measure by embedding the dependence of all realized quantities on the count scale at which the system is probed. The resulting framework preserves standard continuum dynamics in the appropriate limit while introducing a well-defined, scale-dependent deviation at finite count separation.
APPENDIX C: EMERGENT ABELIAN GAUGE STRUCTURE
This appendix derives the Abelian gauge structure directly from conservation of Internal Frame count under the Frames mapping. No independent gauge field, gauge symmetry, or continuum current is postulated. Instead, the gauge sector emerges from the realization of conserved count structure in the System Frame, consistent with the definitions of JI, ϕI, M, ρS, and Ω given in Appx. A.
C.1 Emergence of System Frame Current Conservation from Internal Frame Count Conservation
All realized System Frame conservation laws originate from conservation of measurement availability within the Internal Frame. Let ω'⊂ω denote a finite relational region. The corresponding regional count is
The evolution of this count is governed by the exact regional conservation law
where ∂ω' denotes the adjacency boundary of ω'.
The boundary count-flux is
Equation (C.2) is the fundamental conservation statement. It depends only on relational adjacency and count redistribution and contains no geometric, metric, coordinate, or continuum structure. The quantities JI and ϕI are purely combinatorial Internal Frame objects and must not be interpreted as continuum currents or surface fluxes.
Application of the Frames mapping produces a realized System Frame representation in which conserved count appears as an encoded availability density ρS(,t) together with a corresponding conserved current 𝑺𝑻S(,t). The resulting continuum conservation law is
Equation (C.4) is therefore not primitive. It is the realized continuum image of the discrete conservation structure defined by Eqs. (C.1–C.3).
C.2 Mapping to System Frame
Under the Frames mapping M:ω→ℛ, a relational region ω'⊂ω is realized as a System Frame domain Ω=M(ω'). The conserved Internal Frame count is represented through the induced encoded availability measure as
Equation (C.5) expresses realization of conserved count in the continuum representation. No independent normalization operator is introduced. The correspondence between count and density is determined entirely by the Frames mapping and its induced realization measure. The density ρS therefore represents the realized encoding of conserved count and not an independently postulated physical substance.
C.3 Induced Continuity Relation
Preservation of count under admissible realizations requires that the mapped image reproduce the conservation structure of Eq. (C.2). Differentiating Eq. (C.5) and applying Eq. (C.2) yields
The realized image of the discrete boundary count-flux is represented by the continuum current through
Substitution of Eq. (C.7) into Eq. (C.6) gives
Applying the divergence theorem produces
Since Ω is arbitrary, the integrand must vanish pointwise, yielding
Equation (C.10) therefore follows directly from conservation of Internal Frame count. The continuity equation is not independently assumed. It is induced by the realization of conserved count under the Frames mapping.
C.4 System Frame Current from Internal Frame Flux Realization
The preceding derivation establishes the origin of the realized current JS. Equations (C.2–C.3) define the exact discrete conservation structure within the Internal Frame, while Eqs. (C.5–C.10) define its continuum realization. No additional conservation law is required.
The role of the realized current may therefore be summarized by the mapping relation
where NS(t) denotes the realized count obtained from the mapped Internal Frame transport. The continuum density ρS(,t) and conserved four-current Jμ are subsequently introduced as the continuum realization of this count structure through Eqs. (C.5–C.10), ensuring preservation of the underlying conservation law under the Frames mapping.
Likewise, Eq. (C.3) and Eq. (C.7) together establish the realization of discrete boundary transport as continuum flux,
The realized current therefore represents the mapping-normalized image of conserved adjacency count transport. It is not a primitive geometric object and is not introduced independently of the count structure. Rather, it emerges from the realization of JI under the Frames mapping.
Equations (C.11) and (C.12) serve only as realization definitions and introduce no new dynamics beyond Eqs. (C.2–C.10). The essential result of this section is that the conserved continuum current required for the Abelian gauge formulation originates uniquely from Internal Frame count conservation. Consequently, the gauge structure developed in Secs. C.5–C.10 inherits its conservation properties directly from the underlying discrete count substrate rather than from an independently postulated continuum symmetry.
C.5 Gauge Transformation
Following Sec. C.4, the conserved Internal Frame count flux is realized in the System Frame as the current density
. The next step is to identify the corresponding potential-like quantity generated by the realized encoded availability itself. Consistent with the definitions established in Appx. A and Appx. B, we define the System Frame log gradient availability field as the covariant extension of the previously introduced spatial log gradient availability field,
Here νμ=∂μlnρS, where ρS is the System Frame encoded availability density induced by the Frames mapping. Because νμ is determined entirely by ρS, it is not introduced as an independent gauge potential but emerges directly from the realized encoded availability structure. Consequently, the gauge sector derived below remains rooted in the Internal Frame count conservation established in Secs. C.1–C.4.
To characterize the redundancy of this realized encoding, let λ() be a smooth scalar function on the realized System Frame domain. Consider a multiplicative rescaling of encoded availability,
The quantity
does not represent a new physical count distribution in the Internal Frame. Rather, it is an alternative System Frame encoding of the same realized count structure. Thus, gauge freedom appears only after realization and reflects a redundancy of continuum representation rather than a symmetry of the primitive count substrate.
Applying Eq. (C.13) to the rescaled encoding gives
Using ln(eλρ)=λ+lnρ, this becomes
and therefore
Equation (C.17) is the fundamental gauge transformation obtained within MQ. Its origin follows directly from the logarithmic structure of Eq. (C.13): multiplicative reparameterizations of encoded availability become additive shifts of the realized log gradient availability field.
At this point the connection with conventional gauge theory becomes apparent. The transformation law (C.17) is identical in form to that of an Abelian gauge connection. The realized electromagnetic potential may therefore be identified with the continuum realization of the MQ field νμ, Aμ≡νμ. This identification is not an independent postulate. Rather, Eq. (C.17) demonstrates that the conventional gauge potential corresponds to the realized log gradient availability field generated by the encoded availability density itself. Consequently, the gauge structure is derived from the Frames mapping rather than assumed a priori.
The significance of this result is twofold. First, it explains why gauge freedom appears only in the realized System Frame description. Second, it demonstrates that the Abelian gauge transformation emerges from the same conserved count structure that generated the current conservation law of Sec. C.4. Thus, the potential and current sectors arise from a common underlying count-based substrate.
Notably, this differs conceptually from conventional continuum approaches. In standard electrodynamics the gauge transformation is usually introduced as a symmetry of the electromagnetic potential itself [1,25,35]. In MQ, the transformation arises from the realized encoding of conserved count structure and therefore appears as a consequence of the Frames mapping. Gauge freedom is thus interpreted as a redundancy of realized representation rather than as a primitive assumption.
C.6 Abelian Closure
The gauge transformation derived in Sec. C.5 has the form A→A+∇λ. To verify closure, let two such transformations generated by λ1 and λ2 act successively. Applying λ1 first and then λ2 gives
Reversing the order yields
Since the addition of gradients is commutative, the two compositions are identical. Hence the commutator of the corresponding gauge variations vanishes,
This establishes Abelian closure, 𝒢≅U(1). Here U(1) denotes the one-parameter unitary Abelian group. In the present formulation, its defining property follows directly from the scalar reparameterization freedom of the realized encoded availability density established in Sec. C.5. No non-commuting generators or additional internal structure are introduced.
The closure property is therefore not imposed independently. It follows directly from the realized logarithmic representation of encoded availability embodied in Eq. (C.13) and the transformation law of Eq. (C.17). The Abelian structure arises because the gauge degree of freedom is generated by a single scalar function λ(), whose gradients commute under composition.
This result completes the derivation of the Abelian gauge group from the realized encoded availability structure. The conserved current obtained in Sec. C.4, the log gradient availability field introduced in Sec. C.5, and the closure relation established here all originate from the same conserved Internal Frame count structure realized through the Frames mapping. No independent gauge postulate, symmetry assumption, or group structure is required beyond the admissible realization of conserved count.
C.7 Field Strength Tensor
Equations (C.13–C.20) establish the MQ origin of the gauge potential through realization of encoded availability and its associated gauge redundancy. Having derived the gauge potential Aμ and realized current Jμ from the Frames mapping, the remaining construction follows the standard Abelian field-theoretic development. The spatial gauge potential 𝑨𝑩(,t) introduced above is expressed in relativistic index notation as Aμ, with the associated field strength tensor defined on the realized spacetime domain. To identify the gauge invariant field strength structure associated with the System Frame log gradient availability field A, define the antisymmetric field strength tensor
The tensor Fμν is the realized System Frame field strength constructed from the same encoded availability structure that produces the current and gauge transformation in the preceding subsections. It is therefore not introduced as a primitive object but arises as the antisymmetric differential structure associated with A on the realized domain M(ω'). Under the gauge transformation established in Sec. C.5,
Expanding this expression yields
Since mixed partial derivatives commute, ∂μ∂νλ=∂ν∂μλ, the additional terms cancel identically, giving
. This invariance demonstrates that the field strength tensor is independent of the specific System Frame encoding of availability and depends only on the underlying realized structure induced by the Frames mapping.
Within MQ, this result shows that the gauge invariant field strength structure associated with the emergent Abelian structure follows directly from the log gradient structure of encoded availability. The same Internal Frame count conservation that produces the realized current in Sec. C.4 and the gauge transformation in Sec. C.5 therefore also determines the invariant field tensor without introducing additional degrees of freedom. The antisymmetric derivative construction isolates the gauge invariant structure associated with A by removing the scalar gauge freedom associated with λ, thereby yielding the unique field strength structure consistent with the Abelian closure established in Sec. C.6.
In this way, the emergence of Fμν completes the minimal structural requirements developed in Appx. C for the realization of an Abelian gauge field in the System Frame. The conserved current, the gauge transformation, and the gauge invariant field strength all arise from the same underlying count-conserving structure in the Internal Frame, transported through the Frames mapping and encoded in the System Frame. This establishes that the field strength construction introduced here is not an independent postulate but a direct consequence of the encoded availability framework developed in the preceding sections, consistent with standard continuum formulations of Abelian gauge theory while remaining grounded in count conservation and encoded availability [1,25,31,35].
C.8 Local-Variation Lagrangian
At the electromagnetic demarcation, the System Frame realization of the MQ Action reduces to a functional depending only on local variation of the log gradient availability field. Consistent with the structures established in Secs. C.6–C.7, this variation is encoded through the antisymmetric combination that defines the gauge invariant field strength,
so that all admissible local dynamics are constructed from mapping induced variations alone. The Lagrangian density is therefore expressed directly in terms of this antisymmetric field strength as
which is the unique Lorentz scalar formed from Fμν without introducing additional dynamical structure. This form follows from the requirement that the action be constructed solely from mapping induced local variation and remain invariant under the Abelian gauge transformation derived in Sec. C.5. Because Fμν is itself gauge invariant, the Lagrangian carries no dependence on the scalar re-parameterization λ.
The importance of this expression within MQ is that it completes the emergence of electromagnetic field structure from the same underlying count conservation structure. The conserved current, the gauge transformation, and the invariant field strength have already been obtained without introducing independent continuum postulates. The present Lagrangian shows that the corresponding dynamical functional can likewise be constructed from those same objects, ensuring that the resulting equations of motion are fully determined by Internal Frame count conservation realized through the Frames mapping. This aligns with the standard field-theoretic requirement that dynamics follow from a variational principle while differing in that the functional form is not postulated independently but follows from the previously established structures [1,25,35].
Applying the Euler–Lagrange variation with respect to Aν,
yields
which corresponds to the source-free limit of the electromagnetic field equations. Within MQ, this result arises because the Lagrangian above is constructed solely from the gauge invariant local variation structure encoded in Fμν, without inclusion of a realized current source. The appearance of sources is instead tied to the underlying Internal Frame count flux, which is mapped into the System Frame through the realized current structure established in Secs. C.1–C.4.
To incorporate this more general case, the action is extended by a minimal coupling term
where Jν is the realized System Frame current obtained from the Internal Frame count flux via the Frames mapping. The full Lagrangian then becomes
Variation of this extended action yields the inhomogeneous field equations
so that Eq. (C.27) is identified as the special case of vanishing mapped current, corresponding to regions with zero net Internal Frame count flux.
In this way, the homogeneous and inhomogeneous field equations are both recovered from the same MQ variational principle. The source-free form follows from the gauge invariant Lagrangian built solely from the gauge invariant field strength, while the sourced form arises when the realized current induced by Internal Frame count conservation is included explicitly. These equations therefore demonstrate that, within MQ, the dynamical equations governing electromagnetic field structure arise directly from encoded availability and its mapped current structure, without introducing independent field dynamics beyond those already established by the MQ Action and the Frames mapping.
C.9 Noether Current
Given the induced conservation law obtained in Sec. C.3, the realized System Frame current satisfies ∂μJμ=0, which serves as the continuum conservation constraint associated with realized transport of Internal Frame count flux. The infinitesimal gauge variation derived in Sec. C.5 takes the form δAμ=∂μλ, and the derivative-only Lagrangian introduced in Sec. C.8 is invariant under this transformation, δℒ=0. Under these conditions, Noether’s theorem applies directly, establishing the existence of a conserved current associated with this symmetry [15].
For a Lagrangian depending only on derivatives of Aμ, the Noether current is determined by the standard variational expression
Here the symbol jμ denotes the Noether current associated with gauge symmetry of the derivative-only Lagrangian. This notation distinguishes it from the realized physical source current Jμ introduced in Secs. C.1–C.4, which arises from mapped Internal Frame count transport and appears as the source term in the inhomogeneous field equations. Using the gauge variation δAν=∂νλ and the definition of the field strength tensor together with the Lagrangian structure of Sec. C.8, one obtains
where the overall normalization of the conserved current is conventional and does not affect the conservation relation. Recognizing the antisymmetric combination as the field strength tensor defined in Sec. C.7,
this becomes
The divergence of this current is constrained by the conservation law. Using the anti-symmetry of Fμν together with commutativity of partial derivatives, one finds
The second term vanishes identically due to anti-symmetry of Fμν, and the first term vanishes in the source-free case established in Sec. C.8, yielding
This establishes that the Noether current derived from the gauge symmetry is conserved as a direct consequence of the antisymmetric field structure together with the source-free field equations. Importantly, this current is not identical to the physical source current that appears in the inhomogeneous field equations. Rather, it encodes the conserved quantity associated with the gauge redundancy of the log gradient availability field.
The physical source current arises separately from the realized transport of Internal Frame count flux under the Frames mapping. As established in Secs. C.4–C.5, discrete adjacency transfer in the Internal Frame is described by the count-flux object JI(ξ→ξ',A), whose regional boundary sum defines the exact discrete flux across a relational boundary. Under realization in the System Frame, this conserved count transport is represented by the continuum current density Jμ, defined implicitly by the requirement that the mapped flux reproduce the induced continuity relation. In this sense,
with the corresponding continuum conservation law ∂μJμ=0.
The current Jμ is therefore the physical source current entering the inhomogeneous field equations, whereas jμ is the Noether current associated with gauge symmetry of the derivative-only structure. The two are conceptually distinct: jμ arises from invariance of the Lagrangian under the gauge transformation Aμ→Aμ+∂μλ, while Jμ arises from the realization of discrete Internal Frame count conservation as observable flux in the System Frame.
In this form, the Noether current is expressed entirely in terms of the gauge invariant field strength derived from the log gradient availability field, while the physical source current is grounded in the mapped realization of discrete count transport. The introduction of jμ is therefore appropriate at this stage, as the differential structure required to support index notation has already been established through the mapping-induced derivative operator and the tensor construction in Sec. C.7. The Noether current is not an independent object, but the realized conserved quantity associated with the gauge symmetry of encoded availability, and its conservation is consistent with the System Frame realization of the discrete Internal Frame count conservation law established in Sec. C.1.
This distinction also prepares the transition to the Maxwell-type equations of Sec. C.10. There, the inhomogeneous equations are sourced by the physical source current Jμ, while the gauge invariant conservation structure established here remains encoded in the Noether current jμ. Electromagnetic field structure therefore contains two complementary conserved structures: one arising from gauge symmetry of the local variation Lagrangian, and one arising from mapped realization of discrete count transport.
C.10 Maxwell-Type Equations
The Maxwell-type field equations follow from the gauge invariant field strength established in Sec. C.7 together with the variational structure developed in Secs. C.8–C.9. In particular, variation of the Lagrangian containing the interaction term ℒint=-JνAν yields the inhomogeneous field equation (C.30) which defines the realized System Frame source current Jν. As established in Secs. C.1–C.4, this current corresponds to the continuum realization of conserved Internal Frame count flux under the Frames mapping. The source term is therefore not introduced independently but arises from the mapped transport structure already required by the continuum conservation law ∂μJμ=0.
The second field equation is
where the brackets denote cyclic antisymmetrization over the indices. This relation is not an additional assumption. It follows identically from the definition of the field strength tensor
together with the commutativity of mixed partial derivatives. It is therefore the tensorial statement of the homogeneous Maxwell equations.
The emergence of the Maxwell-type field equations within MQ follows from the structures developed in the preceding sections. The log gradient availability field generates an Abelian gauge transformation under encoded availability rescaling, while the associated antisymmetric field strength provides the unique gauge invariant differential structure. The variational construction of Sec. C.8 yields the inhomogeneous field equation when coupled to the realized current Jμ, and the definition of the field strength tensor yields the homogeneous identity. Together these relations reproduce the standard Maxwell field structure without introducing an independent gauge postulate.
With the gauge potential represented by Aμ, the field strength tensor assumes the standard form and the gauge transformation Aμ→Aμ+∂μλ. corresponds directly to the encoded availability rescaling established in Sec. C.5.
Under this identification, the MQ derived gauge structure coincides with the conventional Abelian gauge formulation. The Maxwell-type equations therefore arise as the continuum realization of encoded availability and mapped count transport under the Frames mapping, consistent with the gauge, current, and field strength structures established in Secs. C.4–C.9 and without introducing additional field degrees of freedom beyond those already contained in the MQ construction.
APPENDIX D: DISCRETE-CONTINUOUS MAPPING AND CURVATURE SCALING
This appendix formalizes the mapping between Internal Frame discrete structure and System Frame continuum curvature and derives the scaling relations that generate the gravitational coupling.
D.1 Metric Normalization
This subsection does not introduce a second mapping beyond the Frames mapping. Its purpose is to state how the coarse-grained emergent metric obtained in Sec. 3.3.2 transforms under the scalar normalization induced by the mapping normalization functional. In standard differential geometry, a constant conformal rescaling preserves the Levi-Civita connection and therefore the mixed-index Riemann tensor and Ricci tensor, while the scalar curvature acquires inverse scaling [18,23,24,26,28].
Let
denote the pre-normalized emergent symmetric rank-2 descriptor obtained from the coarse-grained System Frame encoding and let
denote the normalized metric used in the effective geometric description. Then
where 𝒩(ω') is the mapping normalization functional evaluated on the admissible relational region ω'⊂ω. This quantity is a scalar normalization factor, not an additional map. For the local region under consideration, the normalization is constant,
so derivative contributions vanish identically. It follows that the Levi-Civita connection is unchanged,
and therefore, the mixed-index Riemann tensor is invariant,
Contracting yields invariance of the Ricci tensor,
while the scalar curvature scales inversely because one inverse metric is used in the trace,
The Einstein tensor therefore remains invariant,
This identifies the Einstein tensor as the normalization-stable geometric object under the Frames mapping. The invariance follows directly from the compensating scaling between the metric and scalar curvature and does not require the introduction of additional geometric structure.
For completeness, the line element rescales as
so that null structure is preserved under normalization. This confirms that the conformal class of the metric is unchanged, while the invariant content relevant for coupling resides in Gμν.
Accordingly, metric normalization in MQ is interpreted as a regional scalar rescaling of an already-emergent metric descriptor, rather than the introduction of an independent geometric field. Under constant normalization, the connection and curvature tensors
and Rμν remain unchanged, while the scalar curvature carries the inverse normalization required to preserve invariance of the Einstein tensor.
D.2 Curvature Scaling
The purpose of this subsection is not to introduce a second curvature theory distinct from GR, but to determine how the MQ count structure fixes the scale at which the emergent System Frame geometry couples to matter. The tensorial curvature objects introduced in the prior section belong to the normalized effective metric
and therefore retain the standard geometric structure of GR [18,23,24,28]. From Sec. D.1, constant mapping normalization leaves the Einstein tensor invariant,
Thus, the geometric structure remains unchanged. Any MQ modification therefore enters exclusively through the scale of coupling to matter and not through alteration of the curvature tensors themselves.
In MQ, this scale is fixed by admissibility conditions on the Frames mapping. Normalization, unique realization, and closure restrict the Internal Frame count structure such that only a single invariant combination of the fundamental measures is admissible,
This invariant is not introduced phenomenologically but follows directly from the admissible mapping structure. The quantity θsi is the fundamental MQ invariant associated with the signal-idler measure introduced in Appx. A ([9], Appx. A). Depending on representation, it may appear as an angle, a dimensionless count quantity, or a momentum measure; in the present context it enters through its momentum representation and therefore sets the scale relating realized count structure to gravitational coupling. Consequently, any gravitational coupling must be expressible in terms of θsi together with the realized count separation.
The relevant scale arises from the count-resolved relation linking realized separation to gravitational response. The realized separation is encoded by nL, while the fractional remainder QL captures the discrete-continuous mismatch induced by the Frames mapping. From the right-angle count geometry of Fig. 1, the realized curvature measure associated with a single update A is
which represents the loss of the residual count fraction QL over the realized count separation nL. To connect this count resolved curvature measure with the continuum gravitational description, we equate Eq. (D.11) with the Newtonian gravitational acceleration,
Equation (D.12) serves only as the large-scale correspondence used to identify the continuum coupling. The MQ expression remains the more fundamental relation because it is derived directly from count geometry and remains valid at finite count separation, where non-Lorentz length contraction contributes through the Informativity differential. Substituting the count-resolved separation l=nLlf yields
from which the realized gravitational coupling is obtained as
Equation (D.14) is exact and follows directly from the established MQ count geometry. It provides the curvature scaling law: the effective gravitational coupling is fixed by realized count structure rather than introduced as an independent parameter. The bridge to GR therefore follows directly from the count-resolved geometry.
The effective field equation retains the Einstein-cosmological form,
Here GMQ denotes the realized gravitational coupling obtained from Eq. (D.14), evaluated at the interaction dependent count separation nL, while ΛMQ arises from the scalar structure established in Sec. 3.3.4. Neither quantity is introduced independently. Both are determined by the same discrete kinematic structure.
Equation (D.14) therefore defines a count dependent gravitational coupling. At finite count separation, 2QLnL≠1, and the realized coupling reflects the non-Lorentz length contraction induced by the Informativity differential. In the large count limit, 2QLnL→1, so that G=c3(tf/mf), recovering the macroscopic gravitational constant as the asymptotic limit of the same count-resolved relation. Curvature scaling in MQ therefore arises kinematically from discrete structure rather than from phenomenological parameter assignment.
D.3 Summary
Metric normalization defines a scalar rescaling between Internal and System Frame representations that preserves the Levi-Civita connection and all tensorial curvature quantities while inducing inverse scaling in the scalar curvature. The Einstein tensor remains invariant under this normalization.
The effective geometric field equation therefore retains the standard continuum form, while the coupling and scalar contributions are determined by the count-resolved structure of the Frames mapping. In particular, the gravitational coupling is fixed by Eq. (D.14), so no independent coupling constant is introduced. The geometric structure is thus standard, while its scale is entirely determined by discrete kinematics.
APPENDIX E: EMERGENT GEODESIC DYNAMICS
E.1 Point–particle Action
Once the coarse-grained metric
has been constructed, the motion of a freely falling test particle is represented, in accordance with standard general relativistic practice, by extremization of a worldline action [18,23,24,26,28]. The role of the present subsection is limited to this continuum reduction. It does not introduce a new MQ dynamical postulate but states the point-particle variational problem on the emergent System Frame geometry already derived from the Frames mapping. The reparameterization-invariant point-particle action is
For time-like trajectories, once λ is chosen to be an affine parameter, this action is variationally equivalent to the quadratic form
Equation (E.2) is the affine parameter representation used to derive the geodesic equation. Within MQ, the metric entering Eqs. (E.1–E.2) is not primitive. It is the coarse-grained System Frame metric induced by conserved count structure under the Frames mapping, as established in Sec. 3.3.3 and Appx. D. Thus, the variational structure matches the accepted continuum derivation of geodesic motion, while the origin of the metric differs from GR. The admissible variation of the worldline is taken to be
so that the Euler–Lagrange variation of Eq. (E.2) yields the geodesic equation in the emergent System Frame geometry, as shown in Appx. E.2.
No additional proportionality ansatz for
is introduced here, and no separate normalization integral is required at the level of the point-particle action. Those elements belong to the prior construction of the coarse-grained metric and to the admissibility conditions on the Frames mapping, not to the worldline variational problem itself. The purpose of Eq. (E.1) is therefore to place the emergent MQ metric into the standard geodesic action framework used in GR, thereby providing the bridge between MQ conserved count structure and the continuum definition of free particle motion.
E.2 Geodesic Equation
The purpose of this subsection is twofold. First, it establishes the variational identities required for the MQ action under admissible variations. Second, it demonstrates that the emergent effective metric
, obtained via the Frames mapping and coarse-graining procedure (Sec. 3.3.3, Appx. D), yields the standard geodesic equation under the worldline variational principle introduced in Sec. E.1. No additional dynamical assumptions are introduced. In particular, the effective metric and its scaling properties have already been established (Eqs. D.1–D.10) and are taken as given.
Proposition E.1 (Covariant Divergence Identity)
Let Vμ be a smooth vector field on the System Frame equipped with the Levi–Civita connection compatible with
. Then
Proof.
Using metric compatibility and the definition of the Levi–Civita connection,
The contracted connection satisfies
so that
E.2.1 Integration by Parts Identity
Equation (E.4) implies the curved-space integration-by-parts identity
which reduces to a boundary term and vanishes under standard compact-support or asymptotic falloff conditions.
E.2.2 Application to MQ Variational Reduction
The identity (E.8) is required in the variation of the MQ action developed in Sec. 3.4.3. Applying Eq. (E.8) to the stress–energy contribution yields
which provides the intermediate variational step connecting Eqs. (67) and (68). The result shows that, after removal of the boundary contribution, the variation depends linearly on Vν through the covariant divergence of the stress–energy tensor. This establishes the variational identity required for the conservation analysis and is independent of the point-particle derivation developed below.
E.2.3 Variational Statement
We now consider the independent problem of free-particle motion on the emergent geometry. Starting from the affine-parameter form of the point-particle action (Eq. E.2), with admissible worldline variations defined by Eq. (E.3) and λ chosen as an affine parameter, the stationarity condition δSpp=0 yields the Euler–Lagrange equations
with Lagrangian
E.2.4 Reduction to metric-compatible form
Evaluating the derivatives gives
which is the standard intermediate form obtained from variation of a metric compatible point-particle action. Using the Levi–Civita connection associated with the emergent metric,
and rearranging Eq. (E.12) yields the equation of motion
No additional dynamical variables are introduced in this reduction. The derivation assumes only the effective metric already obtained from the coarse-grained Frames mapping (Appx. D), together with the associated Levi–Civita connection defined by that metric.
E.2.5 Interpretation within MQ
Equation (E.14) is formally identical to the geodesic equation of GR. Within MQ, however, the result serves a different interpretive role. The variational structure, metric compatibility, and geodesic form coincide with the standard continuum description, while the origin of the metric is supplied by the coarse-grained realization of count structure under the Frames mapping (Appx. D, Sec. 3.3.3).
Consequently, Eq. (E.14) establishes that freely falling trajectories in the emergent System Frame follow extremal paths determined by the effective geometry induced by the mapping. The geodesic equation therefore requires no modification relative to GR. The distinction lies in the origin of the geometric quantities entering the equation rather than in the variational principle itself.
Together with the field equation construction of Appx. D, this result establishes the required kinematic consistency of the framework. The same MQ action that yields the emergent gravitational field equations also yields geodesic motion in the corresponding coarse-grained geometry, without the introduction of additional dynamical principles or interaction specific assumptions.
E.3 Origin of Conservation and Curvature in MQ
The purpose of this section is to demonstrate that the geometric structures established in Appx. D and Sec. E.2 – namely the Einstein field equation and the geodesic equation – are consistent with the underlying Internal Frame count dynamics under the Frames mapping M. No additional dynamical assumptions are introduced. Instead, conservation and curvature in the System Frame arise as the continuum realization of discrete count structure already defined within the MQ framework.
E.3.1 Conservation under the Frames Mapping
In the Internal Frame, admissible evolution is governed by adjacency-based count conservation over a relational region ω'⊂ω, as defined in Appx. B.1. Under the Frames mapping M:ω'→ℛ, this discrete conservation law induces, in the continuum limit, a conserved current in the System Frame. Writing the current as Jμ, where uμ=dxμ/dλ is the worldline tangent introduced in Sec. E.2, one obtains ∇μJμ=0, where ∇μ is the Levi–Civita connection associated with
. This conservation law is not postulated but follows directly from count conservation under admissible mappings. In the continuum description, it corresponds to the covariant conservation of energy–momentum. Using the definition of the stress–energy tensor derived from variation of the MQ action (cf. Appx. D and standard variational relations),
the contracted Bianchi identity, ∇μGμν(gsys)=0, together with the Einstein equation established in Appx. D,
implies
Thus, covariant conservation of stress–energy in the System Frame follows from discrete count conservation in the Internal Frame, establishing consistency between MQ and the standard conservation structure of GR.
E.3.2 Explicit Local Form of the General Variational Definition
Equation (E.26) follows from the variational reduction (Eqs. E.19–E.25) under the condition that the matter Lagrangian depends on
algebraically and not through derivatives of the metric descriptor. This is the standard condition under which the Hilbert definition reduces to a local density form. Starting with
take the variation with respect to
,
Apply the product rule,
Under the stated assumption, ℒℳ𝒬 depends on the metric but not its derivatives, so
Also use the standard identity,
Substituting Eqs. (E.21) and (E.22) into Eq. (E.20) yields
Now compare this with
The admissibility of the variation
is not assumed independently here but follows from the MQ variational principle established in Appx. B.4, where admissible variations are restricted to those induced by the Frames mapping and constrained to preserve normalization, unique realization, and holonomy-free closure. As a result, the arbitrariness of
applies within this admissible class, which is sufficient to enforce equality of the integrands. Because
is arbitrary within the admissible class of variations, the integrands must coincide,
Multiply by -2:
which is precisely the explicit local form. The chain of relations is therefore (E.18) ⇒ (E.19-E.23) ⇒ use (E.22) ⇒ compare with (E.24) ⇒ (E.25) ⇒ (E.26) while
remains the general variational definition. This derivation shows that Eq. (E.26) is not an independent definition but the explicit density form of Eq. (E.27) under the assumption that the Lagrangian contains no derivatives of
. If such derivatives are present, additional terms would arise in Eq. (E.26), while Eq. (E.27) remains valid without modification.
E.3.3 Curvature from Mapping Structure
The origin of curvature in MQ follows from the structure of the Frames mapping rather than from a primitive geometric postulate. In the System Frame, curvature is defined through the non-commutativity of covariant derivatives,
The curvature relation (E.28) defines the continuum geometric manifestation of non-integrability in the emergent System Frame. Within MQ, however, the geometric description is not fundamental. The underlying structure remains the conserved count dynamics of the Internal Frame. Under coarse-graining, the mapping-induced realization of that count structure is encoded in the emergent metric
, whose dependence on the underlying count structure was established in Appx. D.
The total count contained within a relational region ω' is given by Eq. (E.29), while local and regional count conservation are governed by Eqs. (E.30) and (E.31), respectively. These relations establish that admissible evolution is constrained entirely by conservation of count and its transport through the relational adjacency structure. The continuum geometric description therefore arises from the realized encoding of this conserved count structure under the Frames mapping.
The curvature scalar and Einstein tensor follow in the standard manner,
Within MQ, the non-commutativity expressed by Eq. (E.28) reflects the failure of global integrability of the Frames mapping. Transport around a closed loop in the mapped domain does not, in general, preserve vector orientation, indicating the presence of nontrivial mapping structure. The source of this structure is the conserved count dynamics of the Internal Frame described by Eqs. (E.29–E.31). Under coarse-graining, the count-preserving evolution of relational configurations is encoded in the emergent metric
, whose dependence on the underlying count structure was established in Appx. D. The resulting metric therefore provides the continuum realization of the discrete conservation structure rather than an independently assumed geometric background.
The curvature scalar and Einstein tensor follow in the standard manner,
and therefore inherit their dependence on the Frames mapping through the metric. Consequently, the Einstein field equation derived in Appx. D is not introduced independently but follows from the mapping-induced geometric realization.
E.3.4 Consistency with the Geometric Limit
The results of this appendix establish correspondence between MQ and the standard geometric formulation of gravitation. The metric
, its associated connection, and curvature tensors arise from the Frames mapping (Appx. D). The Einstein field equation follows from the MQ action with coupling determined by the same underlying structure. The geodesic equation arises from extremization of the worldline action (Eqs. E.10–E.14). The conservation law ∇μJμ=0 follows from discrete count conservation and implies the standard covariant conservation of stress–energy (E.17). The curvature relation (E.28) identifies geometric curvature with the non-integrability represented in the continuum realization of the mapping.
Taken together, these results show that the fundamental structures of GR – metric, connection, curvature, and conservation – are not independent inputs in MQ but arise from a single count-based framework under the Frames mapping. This establishes compatibility with GR while providing a first principles origin for its geometric content, completing the kinematic component of the unification program.
APPENDIX F: UNIFYING THE GRAVITATIONAL AND ELECTROMAGNETIC FRAMEWORKS THROUGH DERIVATION OF ELEMENTARY CHARGE
We begin with an Internal Frame configuration constraint written purely in terms of MQ fundamental measures prior to the Frames mapping. This relation is not introduced as an identity, but as the minimal algebraic template that constrains two count-based descriptors of the same underlying charge configuration. In this form,
the variables b and d are not arbitrary: once physically identified, the relation defines a nontrivial solution space and provides the template from which the fundamental form of elementary charge is resolved. The role of the derivation is therefore to determine the physically motivated substitutions for b and d in the Internal Frame and then reduce the resulting expression to obtain ef.
Using the Shwartz experiments for reference [49], then the base b is the elementary charge ef as a function of the fundamental mass f(mf) relative to its quantum of angular momentum ℏ (i.e., f(mf)/ħ). Note, non-italicized variables represent their determination at the upper count limit. We know that the fundamental momentum relative to theta is θsi=(1/2)lfmf/tf thus, indicating that we divide ħ by two. And we know that f(mf) – the metric differential associated with mf between frames – is the square of mf because of the known relation for the bound mass of a galaxy, Mb=2nL(θsimf)2. Thus, we modify the fundamental momentum relative to the Internal Frame such that lf(mfmf)/2tf, ([9], Eq. AG6). Making the substitutions,
Such that d=θsi, b=efmf2/lf and such that b/d=b-d, then
This expression provides the Internal Frame representation associated with elementary charge. At this stage, the construction is prior to realization in the System Frame. To obtain the realized form, we apply the same mapping procedure previously used for the fine structure constant ([9], Appx. AA). First, we recognize the count transform,
This relation is then used to construct the corresponding System Frame count mapping,
We now bring in the charge mapping,
and with this we map ef into its Planck-like System Frame representation,
We then account for the Informativity differential, which supplies the classical form as measured in the laboratory. Such that Side a equals 1, Side b equals nL and Side c – the hypotenuse – equals nL+QL (Fig. 1), then using the established MQ relation ([9], Appx. D),
we obtain
and thus, the measured value
This yields a concordance of 2.30σ relative to the 2022 CODATA recommended value. Elementary charge is defined as exact equal to 1.602176634 10-19 C for both the 2022 and 2018 CODATA publications [50,51]. When using 2018 values we resolve ec = 1.602176634(31) × 10-19 C which leads us to two important considerations regarding the current synchronicity of existing measurements.
Table IV: 2018 and 2022 CODATA Published Values for Physical Constants [21,22] | ||
Physical Constants | 2018 CODATA | 2022 CODATA |
Fine Structure Constant | 7.297 352 5693(11) × 10-3 | 7.297 352 5643(11) × 10-3 |
Speed of Light m/s | 2.997 924 58 × 108 | 2.997 924 58 × 108 |
Mass of an Electron kg | 9.109 383 7015(28) × 10-31 | 9.109 383 7139(28) × 10-31 |
Bohr Radius m | 5.291 772 109 03(08) × 10-11 | 5.291 772 105 44(82) × 10-11 |
Planck’s Constant J Hz | 6.626 070 15 × 10-34 | 6.626 070 15 × 10-34 |
Electric Constant F m-1 | 8.854 187 8128(13) × 10-12 | 8.854 187 8188(14) × 10-12 |
MQ uses Planck’s relation αp = lfmf/mea0 as the starting point for resolving the underlying value associated with elementary charge. We must apply the effects of the Informativity differential to resolve the classical form of the expression (what is measured in the laboratory). Conversely, the CODATA electromagnetic formulation is expressed as e2 = 2hαε0c. This can expose differences in mutual consistency between measurements of these constants when evaluated within the MQ framework.
Specifically, while the speed of light and the fine structure constant are shared among the two formulations (Table IV), small but non-negligible shifts occur in the electron mass and the Bohr radius across the 2018 and 2022 adjustments. We’ve noted the changed digits in bold. These shifts are not accompanied by a corresponding change in the electric constant, indicating that the two formulations are not identically constrained across datasets. This demonstrates that agreement between formulations is contingent on internal dataset correlations. Without considering the model, there can be inconsistencies. And therein, we recognize three moving components: the electromagnetic demarcation, the physical constants, and the model that relates them (i.e., classical mechanics and the MQ extension of that model). Only when all three are mutually consistent does the framework satisfy the empirical closure conditions considered here.
Table V: Unification Metrics Based on 2010, 2014, 2018 and 2022 CODATA Published Values [48-51] | ||||
Physical Parameter | 2022 CODATA | 2018 CODATA | 2014 CODATA | 2010 CODATA |
Blackbody demarcation | 84.6005393909226 | 84.6005386470751 | 84.6008735037691 | 84.6024796854814 |
Charge coupling demarcation | 84.6005456714292 | 84.6005457002905 | 84.6005456854468 | 84.6005457394615 |
Elementary charge demarcation | 84.6005397940157 | 84.5997166459620 | 84.6101037175028 | 84.6515261213208 |
AvSigma G1,G2,α,ℏ,μ0,ε0,k,e,a0 | 3.016 | 3.776 | 2.787 | 2.0607 |
Highest sigma demarcation | 84.601073606 | 84.600570081 | 84.605810583 | 84.626338778 |
Table V addresses this by evaluating three independent constructions of the electromagnetic demarcation: blackbody radiation, charge coupling, and elementary charge. Each represents an independent empirical estimate of a common underlying interaction scale. The requirement that all three agree imposes two nontrivial closure conditions on the admissible constant set.
Unfortunately, the equality of the three demarcation equations is not sufficient to determine nL from first principles without empirical input. However, it is sufficient to severely restrict the admissible solution space and to test whether a given set of constants is internally self-consistent under MQ. This is reflected in the average sigma concordance. The 2018 CODATA set exhibits the highest internal consistency across the nine-constant system, chosen as each are exposed to the electromagnetic demarcation, which determines the Informativity differential. In contrast, the 2022 update – while improving individual constant precision – introduces a measurable degradation in global consistency, reducing the average sigma by 0.76. This demonstrates that improvements in individual constant measurements do not necessarily translate into improved system-level consistency within the MQ concordance framework.
The “highest sigma demarcation” row should therefore not be interpreted as a direct determination of the electromagnetic demarcation. Instead, it identifies the value of nL that maximizes global concordance for a given dataset. Because this optimum depends on the input constants, it is dataset-conditioned rather than fundamental. For clarity, we do not use the highest sigma demarcation in our concordance analysis (Appx. H), instead using the charge coupling demarcation or a calculation that is most appropriate to individual constant analysis.
Overall, a stronger and more important conclusion can be drawn from this analysis. That is, all three independent constructions, across multiple CODATA epochs, and the global concordance optimization, converge to a narrow interval near nL ≈ 84.60055. This convergence is statistically nontrivial. It indicates that the electromagnetic demarcation is strongly constrained by the joint structure of the physical constants considered here, and that only a narrow region of parameter space satisfies all MQ consistency conditions simultaneously. Thus, while the equality condition alone does not uniquely determine nL, it transforms the problem from arbitrary parameter selection into one of constrained system consistency.
Specifically, MQ allows constants to be evaluated through their collective compatibility with a fixed interaction scale. The electromagnetic demarcation acts as a global consistency constraint across multiple independent physical relationships. MQ redistributes epistemic weight such that no single constant anchors the system and this leads to the central implication. If a unique electromagnetic demarcation is identified through consistency across independent constructions and datasets, then the associated physical constants become jointly constrained by the same underlying structure.
Continuing with the derivation, Eq. (F.6) provides the Internal Frame representation of ef. Equations (F.8-F.10) then supply the nontrivial transform required to map the Internal Frame representation into the Planck-like System Frame quantity ep, and Eqs. (F.11–F.14) apply the Informativity differential to recover the final measured value ec. The role of Eq. (F.8) is best understood as Padé-style in form. The correction is represented by a rational expression whose denominator carries the dominant nonlinear structure. In standard mathematical usage, Padé approximants are rational functions constructed so that their series expansion matches a target expression to a specified order, and they are particularly effective when polynomial truncations fail to capture dominant nonlinear behavior or when denominator structure governs convergence.
The arithmetic structure of Eq. (F.8) is consistent with the count geometry developed elsewhere in the paper. The coefficients are not being introduced as arbitrary fit parameters in the narrative, but are organized around the factor structure of 84, which is already physically distinguished through the electromagnetic count scale.
The expanded factor structure matters here because the coefficients appearing in the denominator correction are naturally read against the same count decomposition: 2, 3, 6, 7, 14, 42, and 84 are all structurally tied to the same count family. Specifically, we find 22×3×7=84. We also note that 6×14=84. This does not by itself establish uniqueness, but it does show that the denominator correction is embedded within the same arithmetic structure used in the fine structure and electromagnetic demarcation constructions. The term 277 is likewise best read as 276+1, where 276 is the established numerator in the electromagnetic count relation nL = 276/θsi, and the additional 1 is the reference count closure built into the right-triangle and count-normalization structure developed earlier in the paper. In other words, this is the A and B in A2+B2=C2. In this sense, the denominator in Eq. (F.8) reflects the same count structural organization appearing elsewhere in the framework. It is organized by the same count logic that governs the rest of the MQ construction. This aligns with the earlier role of the electromagnetic demarcation and with the defined status of nL, nθ, and the Frames mapping in the current term set.
With the above derivations we can now extend the framework to additional electromagnet measures. For brevity, we present only the electric constant, while noting that analogous steps may be applied to the magnetic constant and related quantities. Taking the recommended form for the electric constant and applying MQ transformations, we resolve
To simplify, we define γF to describe the frame transform and the Informativity differential
We then resolve
This yields a concordance of 1.93σ relative to the 2022 CODATA recommended value. Recalling the MQ derivation for the gravitational constant
we obtain the following relation between the two,
We also draw the reader’s attention to an important structural distinction between Planck units and the MQ fundamental measures. Planck units are obtained by dimensional combination of the constants c, G and ℏ to isolate length, time, and mass scales. While this procedure defines a consistent system of natural units, it does not by itself provide a derivational pathway linking these quantities within a single underlying physical mechanism. Their relation is imposed through dimensional analysis rather than arising from an internal structural constraint.
Within the MQ construction, Eqs. (F.24–F.25) provide an alternative route that does not rely solely on dimensional combination. In particular, applying MQ nomenclature to the escape-velocity bound yields a direct relation between fundamental length and fundamental mass, nL = 2nM, establishing an explicit count-level correspondence between these measures. The fundamental quantities are therefore related within a common kinematic framework. Since the difference between Planck units and the MQ fundamental measures is captured by the Informativity differential, this relation can be used as part of the construction leading to the Planck system ([9], Appx. BN).
APPENDIX G: CODATA EVOLUTION OF G AND MQ RELATION STRUCTURE
The MQ framework yields three distinct realizations of the gravitational coupling under the Frames mapping, corresponding to finite-count (electromagnetic-consistent), asymptotic (macroscopic), and Planck-coupled evaluations. The latter reflects evaluation of the Planck-form expression prior to normalization under the Informativity differential. The evaluated values are
As carried out in Ref. [9], Eqs. (22-25),
Table VI: CODATA Adjustments for G* | ||||
CODATA Adjustment | Rec. G m3 kg-1 s-2 | MQ Branch | Residual | σ-deviation |
2010 | 6.67384(80) × 10-11 | Gem | 4.8 × 10-6 | < 0.06σ |
2014 | 6.67408(31) × 10-11 | Gmacro | 2.1 × 10-6 | < 0.07σ |
2018/2022 | 6.67430(13) × 10-11 | GPlanck | 1.0 × 10-5 | ~ 0.08σ |
* CODATA recommended values for the gravitational constant [47-50].
These values exhibit close numerical agreement with successive CODATA recommended values as displayed in Table VI:
The 2010 and 2014 MQ values agree with the corresponding CODATA adjustments to within a few parts following the last significant digit, substantially below the stated experimental uncertainties. This demonstrates that the CODATA sequence exhibits numerical agreement with distinct MQ realizations under the Frames mapping. The resulting question is therefore why successive adjustments exhibit agreement with different count-dependent evaluations.
The CODATA recommended value of G is obtained from a global least-squares adjustment over a heterogeneous dataset of precision experiments. Formally, the recommended value minimizes a weighted sum of residuals of the form
where the weights wi are determined by reported uncertainties and covariance structure. In practice, this procedure can be strongly influenced by a subset of high-weight measurements, so that the solution may be approximated by a weighted mean over a restricted subset of experiments.
The experimental dataset exhibits dispersion exceeding quoted uncertainties, necessitating uncertainty inflation and correlation treatment in the adjustment procedure. As a result, the effective solution may be influenced more strongly by internally consistent subsets of measurements that carry dominant statistical weight.
In the 2010 adjustment, the effective weight was concentrated in static torsion-balance measurements, particularly the TR&D-96 result [52] and the University of Washington (UW-00) measurement [53], together with early HUST determinations [54,55]. These measurements cluster near G ≈ 6.6738 × 10-11 m3 kg-1 s-2, and their combined statistical weight exceeds that of higher-valued measurements. Consequently, the least-squares solution is shifted toward this lower cluster, yielding numerical agreement with the MQ finite-count realization Gem at the electromagnetic demarcation.
By 2014, the inclusion of high-precision measurements employing electrostatic servo and dynamic torsion pendulum methodologies – most notably BIPM-13/14 [36,37] and UCI-14 [56] – introduced a competing cluster near G ≈ 6.6741 × 10-11 m3 kg-1 s-2. These measurements carried statistical weights comparable to or exceeding the earlier torsion balance results. The redistribution of statistical weight toward this higher valued cluster shifted the least-squares solution upward, yielding the 2014 CODATA value in numerical agreement with the MQ asymptotic realization Gmacro.
The 2018 and 2022 adjustments reflect further evolution of the dataset, including high-precision HUST-16 measurements (time-of-swing and angular acceleration) [39], JILA-10 [57], and atom-interferometric approaches [38]. These measurements populate both lower and higher regions while increasing the influence of higher valued measurements in the overall adjustment. After accounting for correlations and uncertainty scaling, the weighted solution shifts further upward to G ≈ 6.67430(15) × 10-11 m3 kg-1 s-2, yielding numerical agreement with the MQ Planck-coupled realization GPlanck.
At this stage, the effective statistical behavior may be interpreted in terms of cluster dominance. Let the dataset be partitioned into clusters Ck, each characterized by a mean Gk and total weight
. The CODATA solution is then approximated by
so that the recommended value tends to track the cluster with the largest effective weight. The observed evolution from 2010 through 2022 is consistent with a shift in statistical influence from lower valued torsion balance measurements toward higher valued measurements associated with servo-controlled, dynamic, and atom-interferometric techniques.
The resulting 2018/2022 value has a right-tail concordance with GPlanck at the level of 1.75σ, based on CODATA uncertainties. Within MQ, this is interpreted as corresponding to evaluation of the coupling prior to normalization under the Informativity differential. Although the CODATA procedure does not explicitly invoke such a construction ([9], Eqs. 21–25), the resulting recommended value exhibits numerical agreement with this count-dependent evaluation.
The key empirical observation is therefore that CODATA adjustments do not evolve monotonically toward a single value but instead reflect changing contributions from measurement groups characterized by differing methodologies and systematic structures. Within the MQ framework, these clusters are interpreted as corresponding to different realizations of conserved count structure under the Frames mapping. “The CODATA recommended value is influenced most strongly by the measurement cluster carrying the greatest effective statistical weight.
Accordingly, within the MQ interpretation, the sequence of CODATA values from 2010 through 2022 is viewed not as progressive refinement toward a unique scalar constant, but as successive selections among MQ realizations associated with evolving experimental weight. The observed numerical agreement between MQ evaluations and CODATA values is consistent with the structure of the experimental dataset and its statistical evaluation, as interpreted through frame dependent realization under the Frames Principle and the Informativity differential.
APPENDIX H: CONCORDANCE ANALYSIS OF THE FRAMES PRINCIPLE
Table VII presents the details of this analysis for the 2022 CODATA recommended values, with additional source measures noted below. Calculations for all results are provided in the supplemental spreadsheet. Eleven implementations of the Frames Principle are evaluated, using source measures listed in the “Calculation” column to predict the corresponding values for measures, with their source measures listed in the “Measure” column. Two constants are NIST recommended as calculated. Digits in parentheses denote standard uncertainty. Labels in the table identify specific points addressed in the notes below. Before that, we examine two measurement structuring quantities: θsi and the electromagnetic demarcation.
MQ expressions are evaluated as functions of θsi and the MQ fundamental measures. The parameter θsi is evaluated from the 2022 CODATA value of the fine structure constant ([9], Appx. AD) and is used as the invariant scalar governing the mapping between count structure and realized observables.
Notably, nLθsi = 276 ([9], Appx. AC), where nL is the count of lf associated with electromagnetic phenomena, corresponding to the electromagnetic demarcation, and θsi is the invariant MQ scalar that may be represented as the radial expansion rate of the universe or as half of the fundamental momentum relative to the System Frame. This relation fixes the count scale at which electromagnetic interactions are realized.
The parameter θsi is then combined with the MQ expression for the Planck-form of the fine structure constant αp, evaluated without the Informativity differential, and with Planck’s expression for the Bohr radius to resolve the fundamental measures. Within MQ, non-Lorentz length contraction arises through the Informativity differential, which follows from discrete Internal Frame count structure and its realization under the Frames mapping. Standard Planck unit constructions do not incorporate this effect explicitly, because they are defined through dimensional combinations of constants rather than through count dependent realization under the Frames mapping. Accordingly, expressions that do not include the Informativity differential are identified as Planck-form quantities. Where contrasted with MQ fundamental measures, denoted by subscript f, Planck units are labeled with subscript p.
The parameter γF denotes the collection of terms associated with the frame transform and the Informativity differential. It characterizes the mapping normalized relation between Internal Frame count structure and its System Frame realization ([9], Eq. AN1). Among its component terms is the Informativity differential term 2QLnL. The remaining components represent the count transform structure induced by the Frames mapping.
Since the 2019 SI revision [58,59], the magnetic constant is no longer an exact defining constant and must be determined experimentally. The electric constant ε0=1/(μ0c2) therefore also carries uncertainty, and the Coulomb ke=1/(4πε0) is a derived quantity rather than a defining constant.
Demarcations describe the interaction count distance nL, expressed in units of lf, associated with a measurement. The electromagnetic demarcation can be resolved using blackbody radiation, charge couplings, or elementary charge using the following expressions ([9], Appx. AB, AE, AO):
An analysis of electromagnetic demarcation estimates shows little relative change across the CODATA publications considered here. The differently resolved demarcation estimates, although numerically similar, arise from physically distinct constructions. We therefore treat the elementary charge construction in Eq. (H.9) as the system level definition used here, while differences among other determinations are attributed to the use of unsynchronized physical constant inputs.
Table VII: Right tail p–value with Corresponding Agreement Sigma for 11 Implementations of the Frames Principle (2022 CODATA)* | ||||||||||
Phenomenon | Exp. | Calculation [a] | Measure [a] | MQ Calculated | Measure | p–value[a] | Pull | σagree | w/oMQ | |
Gravitational Constant (CODATA 2010) m3 kg−1 s−2[b,c] | αmea0c | G | 6.673 844 83(17) 10–11 | 6.673 84(80) 10–11 | 0.995 | 6.04 10–3 | 2.59 | 0.16 | ||
Gravitational Constant ( CODATA 2014) m3 kg−1 s−2[b,c] | αmea0c | G | 6.674 077 94(10) 10–11 | 6.674 08(31) 10–11 | 0.995 | 6.65 10–3 | 2.56 | 0.00 | ||
Gravitational Constant ( CODATA 2018) m3 kg−1 s−2[b,c] | αmea0c | G | 6.674 311 06(16) 10–11 | 6.674 30(15) 10–11 | 0.960 | 5.04 10–2 | 1.75 | 0.00 | ||
Gravitational Constant ( CODATA 2022) m3 kg−1 s−2[b,c] | αmea0c | G | 6.674 311 05(16) 10–11 | 6.674 30(15) 10–11 | 0.960 | 5.04 10–2 | 1.75 | 0.00 | ||
|
|
|
| 0.9999 | 3.97 | 0.20 | ||||
Global Concordance w/o 2018 & 2022 |
|
|
| 0.99996 | 8.98 10–3 | 3.94 | 0.41 | |||
Hubble Constant (SPT–3G) km s–1 Mpc–1[b,c] | αmea0kBhcTCMB | HCMB | 68.259(19) | 68.3(15) | 0.978 | 2.74 10–2 | 2.02 | n/a | ||
Hubble Constant (Pantheon+) km s–1 Mpc–1[b,c] | αmea0kBhcTCMB | Hcepheids | 73.508(21) | 73.5(11) | 0.994 | 7.47 10–3 | 2.51 | n/a | ||
Global Concordance |
|
| 0.9996 | 2.84 10–2 | 3.35 | n/a | ||||
Fine Structure Constant (no length contraction)[d, f] | α | ħε0ec | 137.040 785 6(30) | 137.040 785 623(21) | 0.9997 | 3.46 10–4 | 3.45 | 0.00 | ||
Fine Structure Constant (Classical)[d, f] | α | ħε0ec | 137.035 999 2(30) | 137.035 999 177(21) | 0.9997 | 3.47 10–4 | 3.45 | 0.00 | ||
Global Concordance |
|
|
| 0.9997 | 3.47 10–4 | 3.45 | 0.00 | |||
Half Fundamental Momentum kg m s–1[e] | αmea0c | ħGc | 3.262 390 305(89) | 3.262 390(23) | 0.9999999997 | 3.45 10–10 | 6.20 | 4.79 | ||
πmflf/4γFReduced Planck Constant J s[f] | αmea0c | ℏ | 1.054 571 818(26) 10–34 | 1.054 571 817(13) 10–34 | 0.9998 | 3.04 10–4 | 3.49 | 0.00 | ||
4γF/πmflfc2Magnetic Constant N A–2[g] | αmea0ε0c | µ0 | 1.256 637 063(64) 10–06 | 1.256 637 061 27(20) 10–6 | 0.9730 | 3.39 10–2 | 1.93 | 0.00 | ||
mflfc2/16γFElectric Constant F m–1[h] | αmea0µ0c | ε0 | 8.854 187 80(45) 10–12 | 8.854 187 8188(14) 10–12 | 0.9729 | 3.39 10–2 | 3.93 | 0.00 | ||
ec=2QLnLrne/rqCoulomb Constant Nm2C2[i] | αmea0µ0c | ke | 8987 551 802(458) | 8987 551 786(14) | 0.9729 | 3.39 10–4 | 1.93 | 0.00 | ||
(U90) Elementary Charge C[j] | αmea0µ0c | e | 1.602 176 633(31) 10–19 | 1.602 176 634(98) 10–19 | 0.9891 | 1.36 10–2 | 2.30 | 0.00 | ||
(U91) Gravitational Constant – unification f(μ0) m3 kg−1 s−2[b] | αmea0μ0c | G | 6.674 077 93(33) 10–11 | 6.67408(31) 10–11 | 0.995 | 6.69 10–3 | 2.55 | 0.00 | ||
Gravitational Constant – unification f(ɛ0) m3 kg−1 s−2[b] | αmea0ε0 | G | 6.674 077 93(34) 10–11 | 6.67408(31) 10–11 | 0.995 | 6.69 10–3 | 2.55 | 0.00 | ||
Global Concordance | 0.995 | 2.55 | 0.00 | |||||||
Bohr Radius (gravitational) m[k] | αmea0ħGc | αmea0c | 5.291 772 11(15) 10–11 | 5.291 772 10544(82) 10–11 | 0.9998 | 2.74 10–4 | 3.52 | 0.00 | ||
Bohr Radius (electromagnetic) m[k] | ε0ħmee | αmea0c | 5.291 772 11(41) 10–11 | 5.291 772 10544(82) 10–11 | 0.99999 | 8.36 10–6 | 4.35 | 0.00 | ||
| 0.99999996 | 2.74 10–4 | 5.38 | 0.00 | ||||||
Age of Universe Gyr[l] | αmea0akBhcTCMB | AU | 13.7943(39) 109 | 13.797(23) 109 | 0.909 | 1.14 10–1 | 1.34 | 1.30 | ||
CMB Temperature K[m] | αmea0ac | TCMB | 2.72509(58) | 2.7248(57) | 0.627 | –4.86 10–1 | 0.32 | 0.27 | ||
MQ Star Velocity ve vs MOND velocity vm[n] | α, vm, c | v | 1–(2.10 10–13) | 4.58 100 | 7.25 | n/a | ||||
Dark Domain vs. Dark Energy (Ωdk vs. ΩΛ)[o] | α | ΩΛ | 68.362 416 12(59) | 68.34(84) | 0.979 | 2.67 10–2 | 2.03 | n/a | ||
Unobserved Domain vs. Dark Matter (Ωuobs vs. Ωc)[o] | α | Ωc | 26.788 748 99(59) | 26.73(82) | 0.943 | 7.16 10–2 | 1.58 | n/a | ||
Observable Domain (Ωobs vs. Ωc+Ωb)[o] | α | Ωc+Ωb | 31.637 583 88(59) | 31.66(84) | 0.979 | 2.67 10–2 | 2.03 | n/a | ||
Visible Domain (Ωvis vs. Ωb)[o, p] | α | Ωb | 4.848 834 891(10) | 4.927(86) | 0.365 | 9.05 10–1 | 0.00 | n/a | ||
MQ Tension Solutions (G, H0)[b] | 0.9999999999 | 3.05 10–2 | 6.63 | 0.00 | ||||||
MQ Tests of Length Contraction (𝐺, 𝛼) |
|
| 0.9999998 | 8.99 10–3 | 5.08 | 0.00 | ||||
MQ Tests of Unification (G with μ0, a0, θsi) | 0.99999992 | 6.69 10–3 | 5.24 | 0.00 | ||||||
MQ Physical Constant Solutions (𝐺, 𝛼, 𝜃si, ħ, 𝜀0, 𝜇0, 𝑎0) |
|
|
|
|
| 1–(7.97 10–17) | 3.57 10–2 | 8.25 | 0.00 | |
MQ Observational Domain Solutions (Ω𝑑𝑘, Ω𝑢𝑜𝑏𝑠, Ω𝑜𝑏𝑠, Ω𝑣𝑖𝑠, Ω𝑓) |
|
|
|
|
| 0.93 | 9.09 10–1 | 1.51 | n/a | |
MQ Frames Principle (Includes all 11 implementations) |
|
|
|
|
| 1–(1.1 10–19) | 4.56 10–2 | 8.74 | 0.00 | |
* Data sources are clarified in the label notes. Gray text indicates implementations not included in the Frames Principle assessment.
First published in Ref. [19], the product nLθsi=276 is discussed in Sec. 3.2.2. This product identifies a count structural feature of the MQ construction. This is assessed by noting that θsi and the electromagnetic demarcation estimates are obtained from different source measurements. θsi is derived from α. The demarcation estimates are derived from measures involving ħ, α, or e. Carrying out a statistical concordance assessment of this product using the ħ-based measure gives p=0.9998 (3.49σ).
If continued analysis supports this relation, then θsi and its connection to electromagnetic interaction scales would be interpreted not as independent physical traits, but as mapping derived properties of the MQ count structure. In this interpretation, expansion is characterized by an invariant scalar whose momentum representation is one-half of the fundamental momentum. Because G=QLrc3/θsi, the gravitational coupling relation is tied to the same invariant scalar. A realization with a different scalar value would therefore yield a different gravitational coupling scale. It is also important to distinguish that the expansion described here refers to the mapping realized expansion structure, not to the kinematic motion of galaxies relative to one another.
We now discuss details of the concordance calculations presented in Table VII.
Note a — For clarity, p-values quantify the likelihood, under the null hypothesis that the model is correct, of obtaining a deviation between calculation and measure at least as large as the one observed. In this right-tail convention, small p-values indicate poor agreement, while large values indicate strong agreement. In this analysis, goodness-of-fit tests are evaluated using right-tail statistics that incorporate the degrees of freedom from physically independent experiments. For presentation, p-values are also expressed as agreement sigma, defined as σ=Φ-1(p), where p is the χ2 right-tail confidence. Notably, the “Pull” column presents the commonly used standardized residual, defined as
which provides a signed measure of the deviation between calculation and measurement in units of the experimental uncertainty. A pull near zero indicates close correspondence, while values with magnitude ≥2 typically signal tension with the reported measurement.
The “Calculation” and “Measure” columns identify the source measures used in each expression, allowing predicted values to be traced back to their underlying measurements. The “w/o MQ” column assesses the same expressions after removal of the non-Lorentz length contraction term 2QLnL, which represents the Informativity differential. The MQ fundamental measures, which include this effect, are replaced by their Planck-form counterparts, which do not contain this term, to assess the corresponding classical expression. Use of Planck-form quantities is important because, like the MQ fundamental measures, they combine electromagnetic and gravitational constants in their construction. In other words, the contrast tests whether the MQ contraction term improves concordance relative to the corresponding Planck-form construction.
Note b — The 2022 and 2018 CODATA values for G [50,51] are excluded from the Frames Principle assessment. Their published values are consistent with a calculation in which the adjustment effectively employs Planck-form unit expressions in evaluating the Planck mass ([9], discussion following Table II). We use 2022 CODATA to demonstrate this calculation.
Reproducing this procedure yields a p-value of 0.960 for the reported value, providing numerical support for this interpretation. For comparison, the 2010 value is numerically closest to an electromagnetic determination (p=0.995), while the 2014 value is numerically closest to a macroscopic determination (p=0.995), with both corresponding to physically distinct and experimentally realizable measurement classes. For completeness, we provide calculations of all four published values in Table VII, where QL and nL denote the interaction count distance associated with a given measurement. QL represents the mapping-induced residual component associated with a count nL of lf (Fig. 1):
Using the MQ nomenclature adopted here, the gravitational constant is resolved through two primary measurement pathways: an electromagnetic determination and a macroscopic, gravity-based determination such as a time-of-swing measurement. The second set of expressions evaluates the value of G using the MQ unification expression.
We assess this expression using the electric constant, which is then used to resolve the gravitational constant. We compare the results to both the macroscopic measure of G and its 2022 NIST recommended value. Here G is not italicized because it denotes the upper count limit realization, consistent with the 2014 CODATA publication. In MQ, evaluations at the electromagnetic demarcation are italicized.
Note c — When assessing tensions, we offer two examples (Table VIII), each involving two distinct physical experiments. Because each experiment represents a separate physical implementation with distinct dominant systematics, each is treated as an independent degree of freedom (DoF).
The PANTHEON+ collaboration released a revised arXiv version [21] after the Hubble tension paper [22] had been prepared. The earlier measure indicated a discrepancy of 0.1 km s-1 Mpc-1 relative to the MQ prediction. With the revised values, both the SPT-3G and PANTHEON+ [20,21] measures agree with the MQ calculated values, yielding a global p-value of 0.9996 (3.35σ).
Hubble calculations require the age of the universe ([9], Appx. BI), which is evaluated using the Fixsen CMB temperature study [60] and the calculated 2022 CODATA value for the radiation constant a [50]. We calculate a from the source measures using the NIST recommended definition.
Note d — The fine structure constant α is treated here as a calculated measure. Several studies support its measured value [49,61–65]. In evaluating α, we denote the MQ calculated value as αc and distinguish between the source measurements that underlie its MQ calculation and those used in the experimental determinations (ℏ, ε0, e, c). Because αp is a Planck-form scalar related to αc ([9], Appx. AA), we do not include αp as an independent implementation in the Frames Principle assessment. For clarity, mixed ceiling–floor brackets ⌊x⌉ denote rounding to the nearest integer, a physically significant operation in the discrete Internal Frame.
Note e — No direct measurement exists for the one-half fundamental momentum representation of θsi. Accordingly, θsi is treated here as a calculated MQ scalar. The Shwartz and Harris measurement context yields θsi near 3.26239 rad [49]; an unpublished source reports an uncertainty of ±2 μrad. In the MQ representation, this value is identified with one-half of the fundamental momentum relative to the discrete Internal Frame ([9], Appx. S), while its System Frame representation is dimensionless. We compare the MQ calculation θsi=(lfmf/2tf) relative to a calculated measure of θsi = (ħc3/4G)1/2.
The MQ calculation is resolved using component terms lf, mf, and tf in their System Frame representation. Accordingly, the corresponding discrete Internal Frame measure is resolved using component terms that exclude the Informativity differential. To do so, each component term is evaluated at the upper count limit,
.
Note f — For the reduced Planck constant ħ, we adopt the 2014 CODATA uncertainty for the 2018 and 2022 publications. MQ resolves values at the interaction count distance of a measurement to capture the Informativity differential associated with the discrete Internal Frame. This is evaluated either at the electromagnetic demarcation, at the relevant interaction count distance, or at the upper count limit. Because no independent macroscopic determination of ħ exists analogous to the 2014 gravity-based determination of G, the macroscopic representation of ħ is calculated. We distinguish this in the notation by using italicized ħ for the electromagnetic determination and non-italicized ħ for the macroscopic representation. MQ presentations use this convention for measured or realization dependent terms.
Note g — As of the 2019 SI redefinition, both the electric constant ε0 and Coulomb constant ke are no longer fixed defining constants. They are derived from other SI-defined quantities. The magnetic constant μ0, which was formerly exact, is now experimentally determined through the fine structure constant α and SI-defined constants (e, h, c). Accordingly, ke=1/(4πε0) and ε0=1/(μ0c2) inherit their uncertainties from the same experimental route. For the magnetic constant μ0, we adopt the 2018 CODATA uncertainty when evaluating the 2010 and 2014 publications. The component term γF carries uncertainties inherited from me and a0.
Note h — For the electric constant ε0, we adopt the 2018 CODATA uncertainty when evaluating the 2010 and 2014 publications. The component term γF carries uncertainties inherited from me and a0. As this implementation derives from a measure of μ0, we do not include ε0 in the Frames Principle assessment.
Note i — For Coulomb’s constant ke, we calculate the uncertainty using the 2022 CODATA uncertainty associated with μ0. The component term γF carries uncertainties inherited from me and a0. Because this implementation derives from a measure of μ0, we do not include ke as an independent implementation in the Frames Principle assessment.
Note j — For elementary charge e, we adopt the 2014 CODATA uncertainty when evaluating the 2018 and 2022 publications. The component term γF carries uncertainties inherited from me and a0. Because this implementation derives from a measure of μ0, we do not include e as an independent implementation in the Frames Principle assessment. Prior calculations also carry an interaction count distance, which is effectively established at the electromagnetic demarcation. In those cases, the effect is already contained in the selected source measure, such as μ0.
Note k — The Bohr radius is a calculated measure, for which we provide both gravity-based and electromagnetic implementations. The first implementation combines the MQ expression linking electromagnetic and gravitational quantities with the Planck-form Bohr radius relation. This result is then compared with an MQ expression representing the calculated measure of a0. No direct measurement of a0 is used in this assessment.
The source inputs (α, me, a0, ℏ, G, c) partially overlap with the calculated-measure inputs (α, me, a0, c). Although this is not a sufficiently independent test of a0, the comparison correlates G and ħ with the remaining atomic measures and therefore provides a physically distinct unification check. Thus, we include the test in the Frames Principle assessment.
The Bohr radius corresponds to an interaction count distance of
, or a realized separation nLlf. Accordingly, we compute a0 using the upper count limit to resolve the Informativity differential associated with G and ħ, rather than using values for these measures evaluated at the electromagnetic demarcation (nL|84.60055). When multiple measures are used in the calculation of another measured value, all component measures must be evaluated at the same interaction count distance. By evaluating component terms at the upper count limit, where the Informativity differential contribution is far below the precision of the values involved, the approximation becomes negligible at the stated precision.
For greater precision, macroscopic measurements could in principle be evaluated at their actual interaction count distance. However, in most experiments this distance is not directly measurable. For example, when determining G at a nominal separation of one meter, the length used to define that separation is itself affected by the contraction term being evaluated. Any assumed interaction count distance therefore implicitly carries a contraction factor and can bias the inferred value of G. Because the Informativity differential is negligible at large separations, where experimental configuration permits, the comparison is clarified by evaluating all quantities at the upper count limit. At this limit, the contraction contribution falls well below current experimental uncertainties, allowing a comparison that is not materially affected by unresolvable assumptions about the measurement geometry.
First, when temporal boundary conditions are significant, there exists an upper count bound of 299,792,458 units of lf per increment of elapsed time tf. While the literature often emphasizes the lower physical bound associated with Planck-scale phenomena, MQ treats the corresponding upper bound as physically significant within its count structured framework. This upper bound enters explicitly in MQ applications, including the solution describing stellar motion about galactic centers ([9], Appx. AK).
The second implementation of the Bohr radius uses the CODATA definition as the calculated reference and compares that with the MQ expression, serving in the role of a corresponding measure. The usual procedure is reversed because the MQ expression used here is itself derived from α,a0,me, and c.
In the absence of G, the default determination of these measures is taken at the electromagnetic demarcation, represented here by the electromagnetic determination of ħ. By convention, we adopt the interaction count distance associated with blackbody radiation.
Note l — Prior MQ publications report the age of the universe as a calculated quantity derived from Fixsen’s CMB temperature study, TCMB=2.72548±0.00057 K [60] ([9], Appx. BI) and compare that result qualitatively with other age determinations. In this work, we statistically compare the MQ predicted age with the Planck 2018 result (TT,TE,EE+lowE+lensing) [66]. Application of MQ indicates tension with BAO relative to non-cosmological measures, motivating its exclusion from this assessment. Because the evaluation is strongly affected by the measured age of the universe, we exclude the result from the Frames Principle assessment.
Note m — As with all comparisons here, the agreement sigma represents the consistency between one set of input measures and another set used to calculate a measure or compare with its reported experimental value. We calculate the CMB temperature using the Planck 2018 age result (TT,TE,EE+lowE+lensing), 13.787±0.020 Gyr, thereby comparing the Fixsen and Planck inputs through the MQ expression. This yields an agreement of 0.32σ. Using MQ’s calculated age of the universe, 13.7943±0.0039 Gyr, yields an agreement of 1.34σ.
It follows that the expression can provide a CMB temperature with high concordance, but without a sufficiently precise independent age measure, it cannot support a physically independent evaluation of the Frames Principle. Current age studies are either derived from CMB measurements or remain too imprecise to isolate the contribution of the MQ framework. Accordingly, we exclude this value from the Frames Principle assessment. That said, the calculation offers quantifiable concordance relevant to the observational motivation against inflationary models [67]. We explain.
MQ describes a quantum epoch lasting 363,312 years, during which the discrete Internal Frame cannot resolve whole-unit values external to a realized System Frame (Appx. BE–BG). This geometry prevents the outer boundary of the proto-universe from being represented as a light speed expansion boundary. Referencing discrete external points becomes possible when the universe reaches a radius of
, marking the end of the quantum epoch and the onset of expansion. With a fixed rate of mass accretion,
kg s-1 ([9], Appx. BE), the effective accumulated mass–energy during the quantum epoch, MCMB≙qe, is used to model the CMB and its homogeneous and heterogeneous properties. Here MCMB≙qe is not the measurable mass–energy relative to an observer in the expansionary epoch. A transform
is applied to resolve the corresponding measured quantity MCMB≙ee in the current epoch.
Based on the 2018 Planck study, current analysis indicates a 90.92% confidence that the MQ derived early universe sequence is statistically favored over models requiring a separate inflationary period. The MQ derivation uses four measured values, α,me,a0, and TCMB, together with the defined or derived values used for a,kB,h, and c. While this is not yet definitive, it suggests that the MQ framework may reproduce key features of the observed expansion history without invoking a separate inflationary period.
Note n — The MQ expression for stellar velocity within a galactic potential is necessarily abbreviated here because the spatial mass-density profile of the Milky Way required for the calculation is not available. To proceed, we infer an effective mass density from the MOND-modeled velocity vm [68–69] and use this to compute the MQ predicted effective velocity ve. When ve is compared directly to the MOND velocity curve, the expression demonstrates strong numerical correspondence,
, equivalent to 7.25σ. In this restricted sense, where vm is treated as the observational proxy, the MQ expression reproduces the proxy velocity field.
Physically, the expression interprets the stellar speed as arising from a constrained gravitational response, in which the bound mass Mb of the system is limited by
yielding an effective mass and therefore an effective velocity ve. In kinetic form this reduces to
However, because the MOND velocity vm is both the input used to infer the mass distribution and the comparison quantity for the MQ-predicted velocity, the variables are not statistically independent. Standard goodness-of-fit tests would treat each velocity datum as an independent degree of freedom, which is not satisfied here. For this reason, the stellar velocity result is not included in the Frames Principle assessment.
Note o — Comparison of MQ observational domain fractions with the 2018 Planck TT, TE, EE+lowE results [66] yields a p-value of 0.93 (1.51σ). MQ observational domain fractions geometrically describe the expanding cosmic frame and are therefore not identical to conventional density parameter measures of dark energy, dark matter, the observable universe, and visible baryonic, neutrino, and radiation components. The MQ approach does not directly correspond to the standard cosmological density parameters Ω, so this comparison is not included in the MQ Frames Principle assessment. These quantities instead describe geometrically significant bounds for each fraction.
Note p — The visible fraction of the universe is calculated as equal to 4.848834891(10)%. This fraction includes baryonic matter, neutrinos, and radiation. Using 2018 Planck data indicating a visible fraction equal to 4.927(86)% plus an additional 0.0013% for radiation and neutrinos, we find studies often report a visible fraction closer to 4.9283(86)% [66,70–72]. This indicates a cosmological tension of p=0.355 (0.92σ) relative to the geometry of the expanding frame, with the reported total exceeding the geometric bound.
STATEMENTS AND DECLARATIONS
The author has no relevant financial or non–financial interests to disclose.
The author has no competing interests to declare that are relevant to the content of this article.
DATA AVAILABILITY
All data that support the findings of this study are included within the article. Calculations supporting this article are available with the file name ‘MQSigma.xlsx’ and can be found at: [https://www.researchgate.net/publication/361148724_OnlineResources] under the entry, ‘Online Resources’.
FUNDING
This research has received no external funding.
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