General Relativity as an Emergent Geometry of Discrete Measurement

Jody A. Geiger

Informativity Institute

Chicago, IL USA 60605

Editorial Board Member for Scientific Reports/Nature

jodygeiger@informativity.org

ORCID: 0000–0001–5389–0447

ABSTRACT

This work presents a first principles derivation of the constituent terms of Einstein’s field equation within the Measurement Quantization (MQ) framework. General relativity successfully encodes gravitational dynamics through a continuum field equation, yet its central objects—the metric, curvature tensor, coupling constant, and cosmological term—are introduced at the level of the continuum rather than derived from a more primitive structure. MQ addresses this gap by replacing the assumption of a pre–existing spacetime manifold with a kinematic construction in which all observables arise through the Frames mapping between the discrete Internal Frame and the relational System Frame. Starting from a count–based primitive ontology defined by fundamental measures and conservation relations, we construct a single action functional and corresponding MQ variational principle. Coarse–graining of conserved count structure yields an emergent System Frame metric, while discrete second–difference relations induce curvature. The stress–energy tensor is obtained variationally from the same action, and conservation follows from mapping–induced symmetry structure without independent postulate. The gravitational coupling and cosmological term are derived from mapping–consistent count scaling and global normalization constraints, respectively, rather than introduced phenomenologically. These results assemble into a field equation structurally equivalent to Einstein’s equation in the macroscopic limit, but with all constituent terms arising from a unified kinematic substrate. The formulation therefore provides a reduction of the metric, curvature, coupling, and cosmological contributions to a single underlying action, establishing a coherent first principles origin for gravitational dynamics within the MQ framework.

Keywords: Measurement Quantization, general relativity, cosmological constant, fundamental measures, Planck units, foundations of physics

1. INTRODUCTION

1.1 The conceptual gap in Einstein’s field equation

Einstein’s field equation [1] provides a remarkably successful continuum description of gravitation, encoding the relation between geometry and matter through

Gμν+Λgμν=8πGc4Tμν,
(1)

where gμν defines spacetime structure, Gμν encodes curvature, Tμν represents matter–energy, and the constants G and Λ (Appx. A.7) set the strength and large–scale behavior of the interaction. This equation is uniquely constrained by general covariance and local energy–momentum conservation, and its structure can be derived from the Einstein–Hilbert action [1,2] under standard variational principles. However, this derivation operates entirely within a continuum framework in which the metric field and associated geometric objects are specified at the level of the continuum rather than realized from a more primitive construction.

This leads to a well–recognized conceptual limitation: while the field equation is dynamically consistent and empirically successful, its constituent terms are not reduced to a more fundamental underlying structure. The metric gμν is postulated as a differentiable field on a manifold, the Einstein tensor Gμν is constructed from this field through differential geometry, and the coupling 8πG/c4 and cosmological term Λ enter as independent parameters fixed by observation rather than derived from underlying structure. In this sense, the theory specifies the evolution of geometric structure without a kinematic account of the origin of the metric, coupling normalization, or cosmological contribution.

From a foundations perspective, this gap is distinct from questions of quantization or unification. It concerns the absence of a derivation of the geometric and coupling sectors from a more primitive description of physical measure. Existing approaches – ranging from geometric unification attempts [3,4] to emergent–gravity programs [5–8] – have explored whether spacetime and its dynamics can arise from more primitive structures, but a derivation of all terms in Eq. (1) from a single kinematic construction remains unresolved.

The objective of the present work is to address precisely this point. Within the Measurement Quantization (MQ) framework [9], the aim is not to modify the macroscopic form of Einstein’s equation, but to derive each of its constituent terms from a single kinematic construction based on the Internal Frame, the System Frame, and their connecting Frames mapping, in accordance with the Frames Principle (Appx. A). In this formulation, the metric, curvature tensor, coupling constant, and cosmological term are developed from the coarse–grained realization of conserved count structure under the Frames mapping, thereby providing a first principles origin for the Einstein field equation.

1.2 Prior programs in the literature

The question of whether the gravitational field equation can be reduced to a more primitive structure has a long history, with several distinct programs attempting to unify or derive its geometric content. Early efforts focused on extending the geometric framework of General Relativity (GR) itself. In the Kaluza–Klein construction [3,10], a higher–dimensional metric is introduced such that the five–dimensional Einstein–Hilbert action,

S=116πG(5)∫d5x-g(5)R(5),
(2)

yields both the five–dimensional Einstein field equation and Maxwell’s equations under dimensional reduction [10]. Here R(5) denotes the Ricci scalar [11] of the five–dimensional metric. This construction demonstrates that gravitational and electromagnetic dynamics can be embedded within a single geometric action but does so by extending the dimensional structure rather than providing a reduction of the primitive geometric inputs.

Weyl’s earlier program [4] sought unification within four dimensions by extending the notion of metric compatibility. In Weyl geometry, the connection satisfies

∇λgμν=-2Aλgμν,
(3)

introducing a gauge field Aλ identified with electromagnetism. While conceptually influential as an early gauge–based unification attempt, the resulting non–metricity leads to non–integrable length transport, preventing agreement with observed matter behavior and therefore precluding a viable physical realization.

More recent approaches have shifted toward gauge–theoretic and emergent descriptions of gravity. In gauge formulations [12,13], gravity is treated as a connection theory associated with local symmetry groups, while emergent–gravity programs attempt to derive spacetime dynamics from statistical, thermodynamic, or quantum information principles. A common criterion across these efforts is whether the full structure of GR – including diffeomorphism invariance, equivalence principle behavior, and the field equation – can be realized without introducing independent postulates. In many cases, aspects of this structure are reproduced, but a complete reduction of all constituent terms to a single underlying construction remains unresolved.

The present work is distinguished from these programs in that it does not extend dimensionality, alter metric compatibility, or enlarge gauge symmetry, but instead seeks a reduction of the constituent terms to a count–based kinematic construction defined through the Internal Frame, the System Frame, and their connecting Frames mapping, consistent with the Frames Principle.

1.3 What counts as a successful first principles presentation

A first principles derivation of the gravitational field equation requires more than reproducing its continuum form. The central requirement is that each constituent term arise from a well–defined primitive structure governed by a single action. In particular, the metric, curvature, coupling, and cosmological contributions must not be independently introduced, but must instead emerge from a unified construction in which their interrelations are uniquely fixed a priori. The stress–energy tensor must follow from variation of the same action that governs the geometry, and its conservation must arise from mapping–consistent symmetry and admissible realization structure rather than from an external condition. Finally, the complete field equation must be recovered in the macroscopic limit without the insertion of additional parameters or postulates.

These requirements reflect the standard criteria applied across geometric, gauge–theoretic, and emergent approaches to gravity, where the essential question is whether the Einstein field equation can be derived rather than assumed. Within this context, the MQ framework is constructed to satisfy these conditions through a single kinematic structure. Its primitive content consists of the discrete count domain of the Internal Frame and its realization in the System Frame through the Frames mapping, consistent with the Frames Principle. No metric or geometric structure is specified at the primitive level; only the discrete count domain, adjacency relations, conservation of count, and admissibility conditions on the Frames mapping are taken as primitive. All observable quantities, including those appearing in the field equation, arise only after application of the mapping.

To make this structure explicit, the following subsections develop the mathematical content of the Frames Principle and its consequences for the emergence of measurable quantities.

1.3.1 The Internal Frame, System Frame, and Reference Frame

The MQ framework distinguishes three interrelated constructs through which physical relations are defined. The Internal Frame is a discrete domain in which physical relations are expressed solely in terms of integer counts nLand nT. The System Frame is the realized representation in which these counts are mapped to continuous, measurable quantities. The Reference Frame provides the operational context within the System Frame in which measurements are compared and interpreted and does not constitute an independent primitive structure.

The Frames Principle asserts that physical observables do not reside in any one of these structures independently. Rather, they arise from the mapping-induced relation between the discrete structure of the Internal Frame and its continuous realization in the System Frame, with measurement defined through mapping-consistent relational encoding relative to a Reference Frame. This replaces the conventional assumption that observables are defined directly within a continuum manifold or coordinate system. In MQ, measurable quantities are therefore relational observables obtained through the Frames mapping acting on conserved count structure rather than attributes defined on a pre-existing geometric domain.

Fig. 1. Count of lf describing realized separation in the System Frame, with discrete count evaluated in the Internal Frame. Modified from [b].1.3.2 Right–Triangle Construction and Count Geometry

The count structure underlying the Frames Principle is made explicit through the right–triangle construction shown in Fig. 1. In this representation, Side a defines the reference count and is fixed to a value of unity, establishing the normalization scale for all comparisons. Side b corresponds to the Internal Frame count nL. When multiplied by lf, it defines the discrete count separation associated with an interaction event within the count domain.

Side c, the hypotenuse of the triangle, represents the realized separation in the System Frame. The hypotenuse corresponds to the mapping-consistent realized separation functional in which the Internal Frame count contribution is expressed together with the residual count contribution QL, such that the realized separation is given by the count combination nL+QL (Appx. A.8). The term QL therefore represents the residual count contribution, measured in units of lf, arising from the transition between discrete count structure and continuous realization.

This construction yields a count-resolved relation consistent with the right–triangle configuration, where the orthogonality of Side a and Side b reflects the independence of reference normalization from the discrete count structure, while the hypotenuse encodes realized separation through mapping-consistent normalization. The hypotenuse therefore represents measurable separation as a composite of these independent count contributions together with the mapping-induced remainder.

The role of this representation is not illustrative but operational. It defines the count structure through which MQ expressions are constructed. The separation measured in the System Frame is therefore a mapping-normalized realization of conserved count rather than a direct projection of discrete count and necessarily incorporates the residual contribution QL. This correction encodes the discrete–continuous mismatch inherent in the Frames mapping, and it is this mismatch that ultimately gives rise to the geometric structure developed in subsequent sections.

1.3.3 Emergence of the Discrete–Continuous Mapping

The mapping between the Internal Frame and System Frame introduces a necessary structural effect arising from the incompatibility between discrete count structure and continuous representation. This effect is encoded through the realized separation structure involving nL and the residual contribution QL, which together quantify the mapping-induced deviation between count-defined separation and realized measure. Because a discrete count cannot be represented exactly within a continuous domain, the mapping induces a correction to measured separation.

This correction is purely kinematic. It does not depend on relative motion and is therefore distinct from conventional relativistic contraction effects [14,15]. Its magnitude depends on count scale and diminishes as counts increase, ensuring agreement with continuum descriptions at macroscopic scales. The mapping thus defines a scale-dependent deformation of measured distance intrinsic to the transition between discrete and continuous representations.

A second effect arises from the evolution of count structure under the internal update index A. With each increment of the update index, the realized relational region undergoes a residual count loss QL relative to the Internal Frame reference scale. Because this loss occurs below the reference scale, it manifests as a progressive displacement in realized separation. Under the Frames mapping, this mapping-induced displacement contributes to the curvature realized in the System Frame.

This kinematic origin of curvature can be expressed directly through the mapping structure. Such that

QLlfnLrtf2cθsi=QLc3rθsi=Gr2
(I.1)

(Sec. 2.7), the gravitational coupling follows from the same count-based construction

G=(QLnL)lfc3θsi=(QLnL)lfc32tflfmf=(2QLnL)c3tfmf,
(4)

and represents the mapping-induced contribution associated with the Informativity differential (Appx. A; [9], Appx. D). Here θsidenotes the mapping-consistent scalar normalization governing count realization. Although often written using the symbol θsi, this quantity is context dependent. In specific limiting constructions it admits an angular interpretation ([9], Appx. A), while more generally it corresponds to a normalized half-momentum scale in System Frame units ([9], Appx. Q) and is dimensionless in the Internal Frame ([9], Appx. AX). These representations are fixed by the same underlying mapping normalization and therefore share a single invariant magnitude. A detailed treatment of this identification and its unit structure is given in Appx. F. Importantly, the contraction term is dominant at small count separations and diminishes with increasing separation, recovering classical gravitational behavior in the large-scale limit, consistent with a 3.94σ concordance (Appx. H) against the 2018 and 2022 CODATA recommended values [a].

The significance of this result is structural. Both curvature and coupling arise from the same mapping-induced relation between discrete and continuous descriptions. No independent geometric or dynamical sector is introduced. This establishes the mapping-consistent origin of both curvature and coupling within a single kinematic construction, providing the basis for deriving all terms of the field equation from the MQ action.

1.3.4 Single–action structure and dynamical closure

Because the MQ framework is constructed at the level of first principles, the resulting continuum expressions take forms already familiar from classical theory. The field equations themselves are therefore not altered in their final representation. What changes is the origin and definition of their constituent terms. Rather than being introduced independently at the continuum level, each component emerges from the Frames mapping acting on the underlying count structure. The novelty of the framework therefore lies not in modifying the final form of the equations, but in establishing that all contributing quantities – geometric, dynamical, and cosmological – arise from a common kinematic origin.

To make this origin explicit throughout the remainder of the paper, quantities realized through the Frames mapping are identified by the upright superscript label sys. This notation denotes a System Frame realization obtained from the underlying count structure and should not be interpreted as an independently postulated continuum quantity. Thus, symbols such as

gμνsys
(I.2)

, Hsys, Λsys, and related observables refer specifically to quantities derived through realization of the count configuration under the Frames mapping. The superscript sys therefore serves a dual role: it distinguishes realized System Frame quantities from their corresponding Internal Frame descriptions and identifies their derivational origin within the MQ framework.

Accordingly, whenever a quantity appears with the superscript sys, its continuum form should be understood as the realized representation of an underlying count-based configuration. In particular, metric structure, curvature, stress–energy, coupling, and cosmological contributions are not specified independently, but emerge from the same underlying count relations associated with the right-angle realization structure of Fig. 1. The continuum description is therefore interpreted as a realized representation of a more primitive count-based structure rather than as the starting point of the theory.

With this interpretation established, the dynamical content of the theory is governed by a single action functional defined over the count structure. Denoting the dynamical field by Φ, defined over the coarse-grained realization of the count structure, the action takes the form

Ssys[Ф,gsys]=∫-gsysLMQ(Ф,∂μФ,gμνsys,θsi)d4x,
(5)

where the Lagrangian is constructed from mapping–induced quantities and contains no independently specified gravitational coupling or sectoral decomposition. The MQ variational principle then requires

δSsys=0,
(6)

from which all admissible dynamics follow (see Appx. A for the definition of the MQ variational principle and Appx. C for its implementation within the MQ count functional framework).

The metric emerges through coarse-graining of the count structure under the Frames mapping, yielding a realized metric

gμνsys
(I.3)

in the System Frame without independent specification. Variation of the same action with respect to this emergent metric defines the stress–energy tensor by

Tμνsys≡-2-gsysδSsysδgsysμν.
(7)

Invariance of the action under diffeomorphisms implies the conservation law (Sec. 2.6),

∇μTμν=0.
(8)

In the macroscopic limit, where the discrete count structure admits a smooth representation, variation of the realized action Ssys yields a field equation of the form

Gμνsys+Λsysgμνsys=8πGc4Tμνsys,
(9)

with the cosmological term Λsys determined by the mapping-consistent expansion structure developed in Sec. 2.8 and Appx. E. Equation (9) is structurally identical to Einstein’s expression (Eq. 1), but with each term now defined by the MQ construction: the metric from the realized separation functional, curvature from second-difference structure (Sec. 2.4), stress–energy from variational response (Sec. 2.5) and coupling from the same fundamental measures. The metric, curvature tensor, coupling constant, and cosmological contribution therefore arise from a single mapping-consistent kinematic construction. The distinguishing feature relative to standard GR is not a modification of the continuum equation, but a derivation of its constituent terms from the realized separation structure of the underlying count geometry.

2. METHODS

2.1 Primitive kinematic structure

The MQ formulation begins with a minimal discrete ontology in which no continuum geometric objects are assumed. The primitive structure consists of the Internal Frame, defined as the domain of integer-valued measurement counts, and the System Frame, defined as the realized relational structure in which these counts become continuous observables through the Frames mapping, consistent with the Frames Principle. All physical quantities arise only through this mapping. Neither a metric nor a differentiable manifold is taken as fundamental.

The Internal Frame is specified by a discrete count structure built from three irreducible measures (lf, mf, tf), which define the minimal units of spatial separation, mass assignment, and temporal update, respectively. Physical evolution is represented not by differentiable trajectories but by ordered updates of conserved count on the configuration domain ω, indexed by the Internal Frame update parameter A, which provides a purely kinematic ordering of configurations and does not correspond to a physical time coordinate.

The primitive count state is therefore described by the integer-valued availability count assignment ni(A) on relational cells i∈ω, together with the corresponding regional count

Nω'(A)
(I.4)

on finite relational regions ω'⊂ω, as defined in Appx. A.

The dimensionless parameter θsi enters at this primitive level as a fixed normalization scalar for count separation. In particular, the count nL satisfies

nLθsi=276,
(10)

so that nL = 276/θsi ([9], Appx. AC). This relation defines the fixed count scale associated with the electromagnetic demarcation (Appx. A), but its role here is restricted to specifying normalization of primitive count separation. The discrete count configuration is accumulated over relational regions ω'⊂ω through the regional count

Nω'(A)=∑i∈ω'ni(A),
(11)

which is the basic conserved quantity from which later coarse-grained observables are constructed. At this stage no metric structure is introduced, and no continuum derivative acts on the count variables. The count-to-continuum relation enters only through the Frames mapping,

M:ω→Ω,
(12)

which assigns Internal Frame count configurations to elements of the realized System Frame relational structure. Under this mapping, conserved regional count provides the primitive input from which measurable separations are later realized in a manner consistent with conservation and closure constraints.

These elements – discrete count assignments ni(A), regional count

Nω'(A)
(I.5)

, the fundamental measures (lf, mf, tf), the normalization scalar θsi, and the Frames mapping M – constitute the complete primitive kinematic specification. No independent metric field, connection, or coupling constant is introduced at this level. All continuum geometric structure arises only after realization of the Internal Frame into the System Frame, establishing the foundation for the subsequent variational construction.

2.2 The MQ action and variational principle

The dynamical content of the MQ framework is governed by a single action functional defined on the realized coarse-grained representation of the Internal Frame count structure under the Frames mapping. Let Φ denote the dynamical field encoding realized deviations of the conserved count configuration and let

gμνsys
(I.6)

denote the realized metric structure associated with the continuum description. The action depends on Φ, its realized derivatives, and the metric, with normalization fixed by the mapping parameter θsi, which enters through mapping-consistent normalization rather than as an independently specified coupling parameter.

The defining statement of the theory is that physically realized configurations correspond to stationary configurations under admissible variations. These variations are taken with respect to both Φ and

gμνsys
(I.7)

, subject to the constraint that they arise from consistent realizations of conserved count under the Frames mapping, as required by the MQ variational principle.

Variation with respect to the dynamical field Φ yields the Euler–Lagrange equations in realized form,

∂Lsys∂Ф-∂μ(∂Lsys∂(∂μФ))=0,
(13)

which govern the evolution of the coarse-grained encoded availability field. The derivative operator appearing here is the realized continuum limit of the System Frame of mapping-induced Internal Frame adjacency relations rather than an independently postulated continuum structure. Indices μ,ν label realized System Frame coordinates xμ.

Restricting attention to variations of the realized configuration with respect to the realized metric structure, the first variation of the action takes the form

δSsys=-12∫d4x-gsysTμνsysδgsysμν.
(14)

which defines the stress–energy tensor

Tμνsys
(I.8)

as the functional derivative conjugate to the realized metric structure. This definition is not postulated independently but follows directly from stationarity under admissible variations consistent with the Frames mapping constraints.

This construction enforces a strict single action structure. The degrees of freedom conventionally associated with matter are already contained within the encoded availability structure governed by the MQ Action. Consequently, no independently specified primitive matter action exists, and no fundamental additive decomposition of the form S=Sg+Sm is admitted. While such a separation may appear in the realized continuum limit of the System Frame, it does not correspond to independent fundamental sectors.

The full first variation, combining the realized Euler–Lagrange variation with the metric response, may therefore be written as

δSsys=∫d4x-gsys[∂Lsys∂Ф-∂μ(∂Lsys∂(∂μФ))∂Ф-12Tμνδgsysμν],
(15)

establishing both the field equations and the source tensor as consequences of a single variational structure. The measure

d4x-gsys
(I.9)

is the realized volume element over System Frame coordinates xμ, induced by the mapping normalization acting on conserved count.

At this stage no independent geometric structure, coupling constant, or cosmological term has been introduced. The MQ Action provides a complete dynamical specification in terms of a single functional. The geometric sector – including connection, curvature, and its relation to the stress–energy tensor – emerges only in subsequent sections from the realized metric structure.

2.3 Emergent metric from coarse–graining

We begin with the fundamental observation that the Frames mapping assigns to each discrete configuration a continuous representation in which separations between configurations are preserved under coarse–graining. In the Internal Frame, separation is defined purely as a count relation through the right-triangle count construction illustrated in Fig. 1. The realized hypotenuse count is first given by Side c equal to nL+QL, or equivalently c2=(nL+QL)2. Dimensional separation enters after System Frame realization, where the corresponding finite measurable separation is

l2=(nL+QL)2lf2,
(16)

where nL denotes the Internal Frame count separation and QL is the mapping-induced residual contribution.

Under the Frames mapping, this realized separation admits a continuum representation. Let dl2 denote the local differential realization of separation in the System Frame, where the symbol d denotes the differential operator acting on continuum coordinates. By construction, this quantity is expressible as a bilinear form in the coordinate differentials,

dl2=gμνsys(x)dxμdxν,
(17)

which defines the emergent metric tensor

gμνsys
(I.10)

as the continuum tensor reproducing the mapped local separation functional. The construction provides the local differential encoding of the realized separation defined in Eq. (16) in the continuum limit.

Within the local quadratic approximation, the components of

gμνsys
(I.11)

follow from the second variation of the realized quadratic separation functional l2(x) with respect to coordinate displacements under the Frames mapping. In standard differential form,

gμνsys(x)=12∂2l2(x)∂xμ∂xν.
(18)

For the count-resolved separation considered here, the realized coordinates are obtained from discrete count increments through the fundamental length measure, so that

∂∂xμ=1lf∂∂nμ.
(19)

Because the continuum coordinates arise from discrete count increments through xμ=nμlf, derivatives transform as ∂/∂xμ=(1/lf)∂/∂nμ. Applying two coordinate derivatives therefore introduces a factor

1/lf2
(I.12)

. The quantity differentiated in Eq. (18) is not the linear separation l, but the quadratic separation l2 from Eq. (16),

l2=(nL+QL)2lf2
(I.13)

. Thus Eq. (18) evaluates the Hessian of the squared separation functional. Since

lf2
(I.14)

is constant with respect to the count variables, it factors outside the derivatives, while the remaining second derivative acts only on the quadratic count term

(nL+QL)2
(I.15)

. The factor

1/lf2
(I.16)

introduced by the two coordinate derivatives therefore cancels the explicit

lf2
(I.17)

multiplying Eq. (16), leaving only the second derivative of the count-resolved quadratic separation. Substituting Eq. (16) into Eq. (18) therefore yields the MQ first principles realization,

gμνsys(x)=12∂2(nL+QL)2∂nμ∂nν.
(20)

Equation (20) provides the count-resolved realization of the metric. Its structure reflects the mapping-consistent realization of the right-triangle count construction, with unit normalized reference side, Internal Frame count separation nL, and realized hypotenuse count separation nL+QL. The defining count relation is therefore

1+nL2=(nL+QL)2.
(21)

This relation encodes the mapping between discrete count structure and realized System Frame separation. The metric in Eq. (20) therefore captures the second-order response of the mapping-realized separation functional to coordinate displacement, providing the continuum representation of the underlying count structure without introducing an independent metric field.

2.4 Curvature sector and Einstein tensor

Section 2.3 establishes the emergent metric structure as a derived geometric structure built from the emergent metric within the realized System Frame. Although

gμνsys
(I.18)

is a System Frame tensor field, its dependence remains entirely determined by the realized separation functional l=(nL+QL)lf. Through Eq. (19), continuum derivatives of the metric remain traceable to the underlying count structure. Using Eq. (20), differentiation of the metric gives

∂αgμνsys=∂α(12∂2(nL+QL)2∂nμ∂nν).
(22)

Resolving the coordinate derivative through Eq. (19),

∂αgμνsys=1lf∂∂nα(12∂2(nL+QL)2∂nμ∂nν).
(23)

where lf is the fundamental length introduced in Sec. 1.5 and Eq. (19). Thus, derivatives of the metric correspond to higher-order variation of the realized separation functional under the continuum realization induced by Eq. (19).

The Levi-Civita connection is defined as the torsion-free metric-compatible connection associated with the emergent metric structure. Written in component form, it is

Γμνρ=12gsysρσ(∂μgνσsys+∂νgμσsys-∂σgμνsys).
(24)

Using Eq. (23), the connection becomes

Γμνρ=12lfgsysρσ(∂gνσsys∂nμ+∂gμσsys∂nν-∂gμνsys∂nσ).
(25)

Substituting Eq. (23) into Eq. (24) expresses the connection entirely in terms of the count-resolved metric:

Γμνρ=12lfgsysρσ[∂∂nμ(12∂2(nL+QL)2∂nν∂nσ)+∂∂nν(12∂2(nL+QL)2∂nμ∂nσ)-∂∂nσ(12∂2(nL+QL)2∂nμ∂nν)].
(26)

This expression shows that the connection is generated by third-order variation of the realized separation functional under coarse–graining.

The curvature tensor is obtained from the non-commutativity of the covariant derivative defined by Eq. (24). Using the same connection, the Riemann tensor is

Rσμνρ=∂μΓνσρ-∂νΓμλρ+ΓμλρΓνσλ-ΓνλρΓμσλ.
(27)

The Ricci tensor is the contraction of the Riemann tensor,

Rμν=Rμρνρ.
(28)

The scalar curvature is then obtained by contraction with the inverse emergent metric,

R=gsysμνRμν.
(29)

The Einstein tensor is then given by

Gμνsys=Rμν-12gμνsysR.
(30)

Substituting Eqs. (28) and (29) into Eq. (30) gives the explicit curvature reduction,

Gμνsys=Rμρνρ-12gμνsysgsysαβRαρβρ.
(31)

Equations (22–31) complete the reduction from the emergent metric structure to the Einstein tensor. Since the metric is fixed by Eq. (20), every term in Eqs. (22–31) is constructed from

gμνsys
(I.19)

, its inverse, and its derivatives. The tensor

Gμνsys
(I.20)

is therefore fully determined by the metric generated from the realized separation functional.

The divergence-free identity follows from standard differential-geometric properties of the Levi-Civita connection constructed from Eq. (24). Its contraction gives

∇μGμνsys=0.
(32)

This identity completes the curvature construction and establishes the mapping-consistent origin of the geometric structure.

2.5 Stress–energy tensor from the MQ action

The source term in Einstein’s field equation must be derived from the same kinematic structure that produces the emergent metric and curvature. In the MQ construction, encoded matter content enters through the realized System Frame structure induced by conserved Internal Frame count under the Frames mapping. Accordingly, the tensor

Tμνsys
(I.21)

is not introduced as an independently postulated source term but is derived as the response of the matter contribution to admissible variation of the emergent metric obtained in Sec. 2.3.

The relevant action is the matter contribution to the MQ variational structure. In the realized continuum limit this action is

Smsys=∫d4x-gsysLm.
(33)

Here the encoded matter content is defined on the System Frame through the encoded availability induced by the Frames mapping, and

gμνsys
(I.22)

denotes the emergent metric generated by the count-resolved separation functional. Variation is therefore taken with respect to the emergent metric structure induced by the mapping, rather than an independently postulated geometric background.

Variation of the matter action with respect to this emergent metric defines the stress–energy tensor,

Tμνsys=-2-gsysδSmsysδgsysμν.
(34)

This is the Hilbert stress–energy definition written for the emergent MQ geometry. The distinction from standard GR is not the variational form itself, but the origin of the metric and encoded matter content entering the variation. In MQ, both arise from the same mapping-induced realization structure.

Equivalently, the first variation of the matter action may be written as

δSmsys=-12∫d4x-gsysTμνsysδgsysμν.
(35)

This identifies

Tμνsys
(I.23)

as the tensor conjugate to admissible metric variation in the realized matter structure. The same emergent metric entering the curvature construction in Sec. 2.4 therefore determines the source contribution.

The determinant variation entering the derivation is

δ-gsys=-12-gsysgμνsysδsysμν.
(36)

Using the determinant variation in Eq. (36), the matter-action variation reduces to the standard metric-response form already given in Eq. (35). Comparison of Eqs. (34) and (35) fixes the stress–energy tensor as the variational response of the matter action.

For a local matter Lagrangian whose dependence on the metric is algebraic, this may also be written in explicit density form as

Tμνsys=gμνsysLm-2∂Lm∂gμνsys.
(37)

Equation (37) is not a separate definition, but the local density form of Eq. (34) under the stated assumption that the matter Lagrangian contains no independent derivatives of the metric.

To complete the reduction, the matter field entering Lm must be specified in terms of MQ primitives. In the present framework, this field is constructed from the System Frame realization of encoded availability derived from conserved Internal Frame count under the Frames mapping. The primary object is the encoded availability density ρsys(x), obtained by mapping-normalized realization of count structure over a relational region.

Normalization of ρsys(x) defines the normalized probabilistic description, but the action is constructed from the underlying encoded availability prior to normalization. A convenient representation of the realized matter field is obtained by introducing a phase field S(x), associated with the conserved current structure, and defining the wavefunction form

ψ(x)=ρsys(x)eiS(x).
(38)

This representation encodes the mapping-induced density and current structure and does not introduce additional dynamical postulates. The phase S(x) encodes the conserved current induced by the Frames mapping, while ρsys(x) encodes realized measurement availability.

The matter Lagrangian Lm is therefore a scalar density constructed from ψ(x), its derivatives, and the emergent metric

gμνsys
(I.24)

. Its explicit form is constrained by the requirement that variation under the MQ variational principle reproduces the continuity and current structure induced by the mapping.

To make this dependence explicit, the stress–energy tensor may be written directly in terms of the realized matter field representation. Substituting Eq. (38) into the matter Lagrangian, the stress–energy tensor assumes the form

Tμνsys=gμνsysLm(ψ,∂ψ,gμνsys)-2∂Lm(ψ,∂ψ,gμνsys)∂gμνsys.
(39)

This makes explicit that dependence on matter degrees of freedom is carried through ψ(x), and therefore through the encoded availability density ρsys(x) and phase S(x).

Thus

Tμνsys
(I.25)

is identified as the tensor describing how mapping-realized encoded matter content responds to variation of the emergent metric. The geometry construction (Sec. 2.4) and the matter structure are therefore built from the same underlying realization structure, ensuring that the field equation contains no independently postulated source term.

Notably, the wavefunction representation in Eq. (38) does not introduce quantum dynamics into the gravitational description. The quantities ρsys(x) and S(x) arise deterministically from conserved Internal Frame count under the Frames mapping, while ψ(x) serves only as a compact encoding of the resulting density and current structure. Probabilistic interpretation emerges only after normalization and does not modify the underlying variational construction.

2.6 Conservation law from diffeomorphism invariance

The conservation law follows from the symmetry of the same MQ Action that generates the field equations. No independent conservation postulate is introduced.

Because the total action is constructed as a scalar functional over the System Frame induced by the Frames mapping, it is invariant under admissible diffeomorphisms of the System Frame coordinates. Under an infinitesimal transformation xμ→xμ+ξμ, invariance of the action implies δSsys=0.

Decomposing the total action into geometric and matter contributions, Ssys=Sg+Sm, and applying the MQ variational principle under admissible variations of the emergent metric

gμνsys
(I.26)

, the variation of the matter contribution yields

δSmsys=-12∫d4x-gsysTμνsysδgsysμν,
(40)

consistent with the Hilbert variational definition established in Sec. 2.5.

Under the diffeomorphism-induced variation of the metric,

δgμνsys=∇μsysξν+∇νsysξμ,
(41)

substitution into the variation of the matter action gives

δSmsys=-∫d4x-gsys(∇μsysTνμ)ξν.
(42)

Integrating by parts and using the arbitrariness of ξμ within the admissible class of variations defined by the Frames mapping yields

∇μTμνsys=0
(I.27)

. This condition follows directly from invariance of the MQ Action under admissible coordinate transformations.

The same conservation law follows from the geometric construction. The Einstein tensor constructed from the emergent metric satisfies the contracted Bianchi identity,

∇μGμνsys=0
(I.28)

, which, together with the field equation assembled in Secs. 2.4–2.5,

Rμνρ=12gμνsysgsysαβRαβρ=8πc4(c3tfmf)Tμνsys,
(43)

and equivalently,

Rμνρ=8πtf2(2tflfmf)Tμνsys=4πtfθsiTμνsys,
(44)

ensures consistency between curvature and source under admissible evolution.

Using c=lf/tf and the dimensional relation lfmf=2θsitf, these expressions show that the coupling between curvature and source is fixed by the same mapping-induced normalization that defines the metric. The Einstein tensor

Gμνsys
(I.29)

is determined by the emergent metric and its curvature, while

Tμνsys
(I.30)

is determined by variation of the matter contribution to the MQ Action. The field equation therefore relates two quantities derived from the same underlying conserved count structure.

Within MQ, both relations arise from preservation of conserved count under admissible realizations of the Frames mapping. Covariant conservation is therefore the continuum realization of Internal Frame count conservation.

Importantly, because the stress–energy tensor is defined as the variational response of the matter action constructed from encoded availability (Sec. 2.5), its conservation reflects invariance of the same underlying count structure under admissible mappings. No additional symmetry or conservation principle is introduced beyond those already required by the MQ variational principle.

Thus, covariant conservation of stress–energy in the System Frame is identified as the macroscopic expression of discrete count conservation in the Internal Frame, completing the consistency chain linking mapping structure, variational dynamics, and observable conservation laws.

2.7 Derivation of the gravitational coupling

The gravitational coupling in MQ is not introduced as an external parameter but is fixed by dimensional closure of the fundamental measures together with the continuum normalization of geometric structure generated by the Frames mapping.

The derivation begins with the right-angle construction introduced in Fig. 1, where realized separation in the System Frame is represented by the hypotenuse

l=(nL+QL)lf
(I.31)

. Within this construction, the quantity QL represents the residual count generated by the mapping between the discrete Internal Frame and the realized continuum description. The ratio QL/nL therefore provides the finite-count measure of mapping-induced deformation associated with the realized separation.

In the curvature-resolved regime, this deformation is realized geometrically as gravitational curvature in the System Frame. This identification follows directly from the count geometry of the right-angle construction and the realization dependent structure of mapping-induced deformation.

This identification is supported independently by experiment. As shown in Appx. H, analysis of the non-Lorentz length contraction predicted by the Informativity differential yields a concordance of 5.08σ with measurement. Likewise, comparison of the electromagnetic and macroscopic determinations of Newton’s constant reported in the 2010 and 2014 CODATA adjustments yields a concordance of 3.94σ. These results support the interpretation that the mapping-induced deformation represented by QL/nL corresponds to a physically realized geometric effect.

At finite count, the MQ expression carrying the dimensions of Newton’s constant is therefore written as

QLlfnLtf2cθsi,
(45)

which follows from the finite-count curvature measure together with the primitive dimensional scales and expansion normalization. The quantity QL/nL supplies the local curvature contribution, while

lf/tf2
(I.32)

compliments the radial scaling and c supplies the expansion normalization. The momentum normalization scale θsi closes the dimensional structure.

Using the MQ fundamental relation θsi=lfmf/2tf, the finite-count curvature expression may be rewritten as

QLc3rθsi≈Gr2,
(46)

which places the result in a form directly comparable to the Newtonian curvature relation G/r2. Here θsi acts as the normalization parameter connecting radial expansion, momentum, and gravitational curvature through dimensional closure of the fundamental measures.

At this stage it is useful to distinguish the notation used for Newton’s constant. Within MQ, the symbol G denotes the upper-count limiting value, G=c3(tf/mf), which is independent of realization scale. When finite-count effects are retained, the gravitational coupling includes the realization-dependent factor 2QLnL, corresponding to the Informativity differential and associated non-Lorentz length contraction. In this case the quantity is written in italics as Gsys to indicate realization dependence.

Substituting r=nLlf then

G=QLrc3θsi=QLnLlfc3θsi=2QLnL(lftf)3(tfmf),
(47)

where all factors are expressed in terms of the primitive measures lf, mf, and tf, together with the normalization scale θsi. This isolates the explicit realization dependence of the finite-count gravitational coupling.

Taking the upper count limit removes dependence on discrete realization scale,

G=limnL→∞2QLnL(lftf)3(tfmf)=c3(tfmf),
(48)

which is finite, realization independent, and consistent with the MQ Planck-scale relation G=c3tp/mp (Appx. B). The gravitational coupling is therefore fixed uniquely by the fundamental measures and carries the correct dimensions, [G]=L3/MT2, without introducing an independent gravitational parameter.

Moreover, the geometric construction and the encoded matter content arise from the same underlying MQ framework and are realized on the same emergent System Frame metric. The geometric contribution defines the normalization of curvature through

Sgsys=c416πG∫d4x-gsysRsys,
(49)

while the matter contribution produces

Tμνsys
(I.33)

through metric variation of the MQ Action. In this representation, Eq. (49) is the continuum form of the geometric contribution obtained after coarse-graining of the MQ Action.

Accordingly, the coupling between curvature and the stress–energy tensor is determined entirely by dimensional closure of the fundamental measures established by the upper count limit in Eq. (48). No additional normalization or adjustment is required. The gravitational coupling appearing in the field equation is therefore a direct consequence of the MQ construction.

2.8 Derivation of the cosmological term

The cosmological term in MQ arises from the global evolution of conserved count under the Frames mapping. In contrast to the standard approach, where Λ is introduced phenomenologically in the Einstein–Hilbert action, the MQ construction derives the scalar contribution directly from invariant properties of the expanding count geometry. The scalar contribution is expressed in terms of the fundamental expansion parameter θsi (Appx. G) as

ΩΛ=θsi2-2θsi2+2,
(50)

where this identification follows from the mapping-consistent scalar expansion definition and preserves normalization under the invariant expansion condition. The corresponding expansion rate is given by (Appx. D)

Λsys=πθsiAU(km/Mpcs/y109),
(51)

where Hsys denotes the System Frame realization of the expansion rate fixed by mapping normalization. This expression represents the unit-resolved form of the scalar expansion H=θsi ([18], Eq. 61) under mapping-consistent normalization and a spatially flat cosmology (k=0) as required by the invariant expansion condition and the mapping-consistent realization of the metric. The implied expansion rate is in 3.35σ concordance with observational constraints (Appx. H), specifically the SPT-3G analysis [16], the Pantheon+ cosmological analysis [17], and the MQ Hubble tension analysis [18].

Within the standard FLRW parametrization, the MQ scalar may be identified with the cosmological density parameter for comparison with observational cosmology through

ΩΛ=ρΛρc=Λsysc2/(8πG)3H02/(8πG)=Λsysc23H02,
(52)

with

ρc=3H02/(8πG)
(I.34)

, where G includes the MQ-predicted non-Lorentz length contraction. This relation provides a comparison bridge to standard cosmological notation and does not constitute an independent derivation of the MQ scalar.

Combining Eqs. (50–52) yields

Λsys=3(πθsiAUckm/Mpcs/y109)2θsi2-2θsi2+2.
(53)

Thus, within MQ, the cosmological term is fully determined by mapping-consistent quantities and contains no independent scalar parameter. Unit conversions are retained explicitly for clarity of the derivation. This is discussed further in Appx. F.

The scalar therefore enters the gravitational description as a consequence of the expansion structure defined by θsi and realized through Hsys. The normalization factors arising from the Frames mapping cancel identically in the construction, fixing the scalar contribution through the same closure conditions that determine the geometric and matter contributions.

This construction resolves the status of Λ within MQ. The cosmological term is not introduced at the level of the action nor fixed phenomenologically. Instead, it is a derived scalar determined by invariant properties of the Internal Frame count structure under the Frames mapping. Its value is fixed for a given realization of the mapping, while its origin is kinematic and tied to the expansion structure encoded in the mapping.

Although Λsys appears constant at the level of the realized field equation description, consistency with the conservation law derived from diffeomorphism invariance (Sec. 2.6), ∇μTμν=0, requires that any evolution in the realized scalar contribution be balanced by corresponding evolution in stress-energy under expansion.

The construction is therefore structurally closed: the cosmological term is determined within MQ by ΩΛ, Hsys, and the FLRW density identification in Eq. (52), with its magnitude fixed by Eq. (53). Its embedding in the gravitational description follows from the mapping-consistent realization of the metric and stress-energy tensor developed in Secs. 2.3–2.6.

2.9 Assembly of the field equation

We now assemble the MQ field equation in terms of the fundamental measures (lf,mf,tf) and θsi, presenting its fully reduced form. At this stage, the metric is already established as an emergent, coarse-grained System Frame object induced by the Frames mapping. The curvature follows from this metric as developed in Secs. 2.3–2.4, while the stress-energy tensor is defined variationally with respect to it, ensuring a consistent geometric and dynamical structure. The gravitational coupling (Sec. 2.7) and the cosmological term (Sec. 2.8; Appx. E) have likewise been derived from the same fundamental measures. With these components fixed, the field equation follows by direct composition.

We begin by introducing the geometric tensor entering the MQ field equation. The curvature tensors entering the field equation are constructed from the emergent metric

gμνsys
(I.35)

derived in Sec. 2.3 using the standard Levi–Civita connection [19]. The Riemann tensor

Rσμνρ
(I.36)

[20,21] is formed from this connection, with the Ricci tensor [22] and scalar curvature given by

Rμν=Rμρνρ
(I.37)

and

R=gsysαβRαβ
(I.38)

, respectively. Indices are raised and lowered using

gμνsys
(I.39)

. Then,

Gμνsys=Rμν-12gμνsysR,
(54)


which expresses the geometric tensor entirely in terms of the primitive measures and the normalization scalar θsi. Because

gμνsys
(I.40)

is fixed by the coarse-grained realized count structure defined in Sec. 2.3 from Eq. (20),

gμνsys(x)=12∂2(nL+QL)2∂nμ∂nν,
(55)

the connection, Riemann tensor, Ricci tensor, scalar curvature, and Einstein tensor

Gμνsys
(I.41)

defined in Eq. (54) are all determined by successive derivatives and contractions of the same mapping-realized count structure.

The stress-energy tensor entering the field equation is defined variationally by

Tμνsys=-2-gsysδSmδgμνsys.
(56)

This tensor arises from the count–geometry coupling under the MQ variational principle. The cosmological contribution is likewise fixed within MQ. From Appx. E, particularly Eqs. (E.1–E.7),

Λsys=3(πθsiAUc(km/Mpcs/y109))2θsi2-2θsi2+2.
(57)

Using Eq. (48) together with the dimensional closure relation lfmf=2θsitf (Eq. B.1), the Einstein field equation coupling becomes

8πGc4=8πc4c3tfmf=8πtf2lfmf=4πtfθsi,
(58)

where the reduction uses the MQ expression for the gravitational constant

G=lim⁡nL→∞2(QLnL)c3tf/mf=c3tf/mf
(I.42)

, and the fundamental expression lfmf=2θsitf, eliminating all intermediate scale dependence. Substituting Eqs. (54–58) then yields the assembled MQ field equation

Rμρνρ=-12gμνsysgsysαβRαρβρ+3(πθsiAUc(km/Mpcs/y109))2θsi2-2θsi2+2gμνsys=4πtfθsi(gμνsysLm-2∂Lm∂gμνsys).
(59)

For compact notation, define the MQ coupling by

Ksys=8πGc4=4πtfθsi.
(60)

Then, Eq. (59) may be written equivalently as

Gμνsys+Λsysgμνsys=KsysTμνsys.
(61)

This completes the first principles assembly of Einstein’s field equation within MQ. The curvature term is constructed from the emergent System Frame metric, the scalar term is fixed by the mapping-consistent expansion structure, the source term is obtained variationally from the matter action, and the coupling is reduced to the fundamental measures. No independent Newton constant, cosmological parameter, or external stress-energy source is introduced.

Because Λsys depends on the expansion scale AU (Appx. A.6; Appx. D), Eq. (61) implies that any realized evolution in the scalar contribution must be accompanied by compensating evolution in

Tμνsys
(I.43)

, while G remains fixed kinematically by (lf,mf,tf,θsi). The geometric tensor

Gμνsys
(I.44)

likewise cannot arbitrarily adjust to offset such evolution.

This behavior is consistent with the covariant conservation law, ∇μTμν=0, which requires evolution in the realized scalar contribution to be balanced by corresponding evolution of the stress-energy content. Because all remaining quantities in Eq. (61) are fixed by kinematics, the required decrease in

Tμνsys
(I.45)

implies dilution of energy density under expansion. Within MQ, this excludes static realizations and implies expansion from a finite realization origin consistent with the realized count structure.

3. RESULTS

3.1 Term–by–term reduction of Einstein’s equation

The assembly of the MQ field equation in Sec. 2.9 establishes more than a formal correspondence with GR, providing a term-by-term reduction of Einstein’s field equation in which each constituent term is realized from a common kinematic origin defined by conserved Internal Frame count under the Frames mapping. This resolves the central gap identified in Sec. 1.1: while standard GR is dynamically complete, its constituent terms are introduced at the continuum level rather than derived from a shared primitive structure. Within MQ, Einstein’s equation is not modified at the macroscopic level but reinterpreted structurally, with all terms emerging as mapping-induced realizations of conserved count. In contrast to the Einstein–Hilbert formulation, which derives field equations from a specified action once the metric, coupling, and matter content are defined, MQ derives the origin of these terms (Table I) prior to assembling the field equation, establishing closure within the MQ framework in which no term entering Eq. (61) is independently introduced.

Table I: Term–by–term reduction of Einstein’s equation under MQ

GR Term

MQ Realization

Origin in MQ

gμν
(U.1)

Emergent System Frame metric

gμνsys
(I.46)

, defined as the coarse–grained realization of the separation functional induced by the Frames mapping.

Sec. 2.3

Gμν
(U.2)

Einstein tensor constructed from

gμνsys
(I.47)

through the mapping-induced connection, Ricci tensor, and scalar curvature.

Sec. 2.4

Tμν
(U.3)

Variational response of the matter contribution of the MQ Action with respect to

gμνsys
(I.48)

, with matter represented through encoded availability.

Sec. 2.5

8πG/c4
(U.4)

Reduced MQ coupling κsys, fixed by dimensional closure of (lf, mf, tf, θsi).

Sec. 2.7; Sec. 2.9

Λgμν
(U.5)

Scalar contribution

Λsysgμνsys
(I.49)

, fixed by ΩΛ, Hsys, and the FLRW density identification.

Sec. 2.8; Eq. (57); Appx. E


The metric

gμνsys
(I.50)

arises as the coarse-grained realization of the separation functional induced by the Frames mapping, ensuring consistency with its definition as a relational encoding rather than a fundamental manifold. Curvature follows as the continuum realization of discrete second-difference structure induced by adjacency relations in the Internal Frame. This ensures that geometric curvature reflects accumulated mapping-induced deformation. The stress-energy tensor is defined variationally from the MQ Action, preserving its standard functional role while eliminating the need for an externally supplied source term. The gravitational coupling is fixed by dimensional closure of the fundamental measures (lf, mf, tf, θsi), and the cosmological contribution is determined by the expansion parameter θsi through the associated scalar density fraction ΩΛ.

Several longstanding structural questions regarding Einstein’s equation are addressed by this reduction. First, the origin of geometry is recast as mapping-induced rather than fundamental, with spacetime structure arising from the realization of discrete count relations in the System Frame. Second, conservation of the stress-energy tensor follows directly from mapping-consistent invariance of the MQ Action, ensuring that geometric and matter contributions are jointly constrained by a single variational structure. Third, the gravitational coupling is no longer introduced as an independent phenomenological parameter. Fourth, the cosmological contribution is fixed by the same kinematic structure governing expansion, addressing the ambiguity in interpreting Λ as either vacuum energy or a geometric constant.

The completed Eq. (61) therefore represents a closure statement: the full Einstein field equation is obtained without introducing an independent spacetime manifold, independent matter source, free gravitational coupling, or phenomenological cosmological parameter. All terms are derived from the MQ Action under the constraints of the Frames mapping, and each admits a mapping-consistent realization in the System Frame. In this sense, the apparent equivalence between MQ and GR at the level of field equations reflects a deeper reduction in which the continuum description emerges as a coarse-grained limit of discrete kinematics.

This result does not alter the empirical content of GR. Instead, it provides a first principles account of why Einstein’s equation takes its observed form. The standard field equation remains the macroscopic continuum description, while MQ specifies the underlying structure from which that description emerges. Any measurable departure from GR must therefore originate from count-resolved realizations encoded in the mapping and become observable only outside the large-scale continuum regime.

3.2 Recovery of the standard macroscopic form

With the MQ field equation assembled in Sec. 2.9, recovery of the standard macroscopic form consists in demonstrating that System Frame quantities converge to their general relativistic counterparts in the continuum limit defined by large count separation under the Frames mapping. No additional assumptions are required beyond those already encoded in the MQ Action and its variational structure.

The metric

gμνsys
(I.51)

, defined as the coarse-grained realization of the separation functional, satisfies the smoothness and differentiability conditions required for continuum geometry when evaluated over regions large compared to the fundamental count scale. In this regime, the discrete adjacency structure admits a consistent coarse-grained limit, and the metric becomes operationally equivalent to a continuum spacetime metric at observational resolution.

The curvature follows accordingly. The Einstein tensor

Gμνsys
(I.52)

, constructed as the continuum realization of the discrete second-difference operator on the Internal Frame adjacency structure, reduces to the standard curvature tensor of differential geometry. Its divergence-free property,

∇μGμνsys=0
(I.53)

, is recovered as the continuum realization of mapping-induced conservation constraints, consistent with the contracted Bianchi identity [22].

The stress-energy tensor

Tμνsys
(I.54)

, defined variationally from the MQ Action, retains the standard conservation law,

∇μTμνsys=0
(I.55)

, as a direct consequence of mapping-consistent invariance.

The coupling constant Ksys=8πG/c4, derived from dimensional closure of the fundamental measures, numerically converges to the empirically inferred gravitational constant in the macroscopic regime in which measurements probe separations far above the fundamental count scale.

The cosmological contribution likewise retains its standard form. The scalar term

Λsysgμνsys
(I.56)

, fixed by the mapping-consistent expansion structure, enters the field equation identically to the general relativistic cosmological term. At macroscopic scales, any residual dependence on discrete structure is suppressed below observational sensitivity, leaving only the fixed effective value of Λsys.

The recovery is therefore exact at the level of the continuum field equation. Any deviation between MQ and GR arises only through count-resolved corrections encoded in the Frames mapping, which are parametrically suppressed in the large-scale limit relevant to classical gravitational phenomena.

This establishes that Einstein’s field equation is realized as the continuum limit of the MQ kinematic framework rather than introduced as an independent postulate, while preserving its empirical content in the macroscopic regime.

3.3 Internal consistency checks

The recovery of the macroscopic field equation in Sec. 3.2 establishes structural equivalence with the Einstein formulation. The present section verifies that this equivalence is dynamically and kinematically self-consistent by demonstrating that the internal constraints of GR arise from the Frames mapping acting on conserved count.

The geodesic limit may be stated equivalently through the standard point-particle action evaluated on the emergent metric constructed in Sec. 2.3.

Sppsys[xμ(λ)]=-m∫dλgμνsys(x)ẋμẋν,
(62)

or, for an affine parameter

S'ppsys=m2∫dλgμνsys(x)ẋμẋν.
(63)

Variation with fixed endpoints gives

d2xμdλ2+Γαβμ(gμνsys)dxαdλdxβdλ=0.
(64)

These relations establish that extremization of the mapping-realized action yields the geodesic equation associated with the emergent metric and its metric-compatible connection derived from

gμνsys
(I.57)

. Since

gμνsys
(I.58)

is constructed in Sec. 2.3 and the connection is fixed in Sec. 2.4, this identifies localized motion in the coarse-grained System Frame with extremal curves of the realized metric.

The first requirement is the geodesic limit, which in MQ follows from conservation. In GR, free motion follows from covariant conservation of the stress-energy tensor together with the contracted Bianchi identity. In MQ, the corresponding result follows from conservation of adjacency flux in the Internal Frame, which under mapping normalization induces a conserved current in the System Frame, yielding

∇μTμνsys=0
(I.59)

as the continuum realization of count conservation. For localized distributions, this conservation condition implies geodesic motion in the emergent metric.

The second requirement is compatibility between conservation and the field equation. In GR, the identity ∇μGμν=0 ensures consistency with energy–momentum conservation. Within MQ, this identity arises from invariance of the mapping-normalized metric under admissible transformations, so that the Einstein tensor constructed from

gμνsys
(I.60)

satisfies the same divergence-free condition.

The third requirement is invariance structure. The Einstein equation is invariant under diffeomorphisms of the spacetime manifold. In MQ, the continuum analog arises from automorphisms of the mapping domain that preserve normalization, repeatable realization, and closure. These transformations induce a symmetry on realized configurations equivalent to diffeomorphism invariance in the continuum limit.

The fourth requirement is frame-scaling consistency. The Frames mapping induces a normalization relating Internal Frame count representation to its System Frame realization. In the homogeneous limit this normalization reduces to a constant background factor, while more generally it is fixed by mapping constraints over the relational region. Physical observables must remain invariant under this transformation. Substitution into the MQ field equation shows that all normalization factors cancel identically, yielding a representation independent relation.

Taken together, these results establish that geodesic motion, conservation, invariance, and scaling consistency arise from preservation of conserved count under admissible mappings, reproducing the internal consistency structure required of GR in the continuum limit without introducing additional dynamical assumptions.

4. DISCUSSION

4.1 What is genuinely reduced to first principles

The preceding sections establish that the macroscopic field equation obtained from MQ is structurally equivalent to the Einstein equation, while its constituents arise from a single underlying kinematic construction. The present section isolates the structures reduced to first principles within this construction and distinguishes them from the elements that remain primitive.

The fundamental statement is not a field equation but the variational condition on the MQ Action, defined entirely on the Internal Frame configuration domain and its admissible Frames mapping. At this level, no metric, connection, curvature tensor, or stress–energy tensor is introduced. The primitive content consists only of the discrete configuration domain, adjacency-defined transport, conservation of count, and admissibility constraints on the mapping, including normalization, repeatable realization, and holonomy-free closure.

From this structure, the objects treated as fundamental in GR are derived. The metric

gμνsys
(I.61)

arises as the coarse-grained realization of the separation functional induced by the mapping, with its scaling fixed by normalization of conserved count rather than coordinate choice. The associated connection and curvature tensors follow from the continuum limit of the induced second-difference structure encoded in adjacency relations, yielding the standard geometric form without additional postulates.

The stress–energy tensor is likewise not introduced phenomenologically. It is defined variationally from the matter contribution to the MQ Action through variation with respect to

gμνsys
(I.62)

, with the matter sector expressed through encoded availability and its normalization. Geometry and source therefore arise from the same functional structure.

The gravitational coupling is reduced to the dimensional structure of the fundamental measures (lf, mf, tf, θsi), with its value fixed by mapping-consistent scaling relations. The cosmological contribution is determined by the MQ expansion sector through ΩΛ, H0, and the associated MQ cosmological contribution, rather than introduced as an independent phenomenological parameter.

Taken together, these results imply that the field equation is not fundamental but a derived consistency condition on the realization of conserved count under the admissible Frames mapping. Each term in the macroscopic equation is fixed by Internal Frame count structure and its realization in the System Frame.

What remains primitive is correspondingly minimal: the configuration domain, adjacency-defined transport, conservation of count, and the admissibility conditions defining the Frames mapping. These are not derived within the present framework.

By contrast, the continuum structures of GR – the metric, connection, curvature, stress–energy tensor, coupling constant, and cosmological contribution – are secondary. They arise as continuum representations of conserved count realized in the System Frame, consistent with the Frames Principle.

The reduction achieved is therefore structural. The continuum description of gravitation is retained in standard form, but its constituent elements are reinterpreted as emergent from a single discrete kinematic structure governed by the MQ Action.

4.2 Relation to GR

The relationship between MQ and GR is one of structural equivalence at the macroscopic level combined with a difference in foundational origin. The MQ framework does not modify the Einstein field equation within its established domain of empirical validity but reproduces its standard form as the continuum realization of a kinematic structure defined by the Frames mapping.

At the level of observable physics in the System Frame, gravitational dynamics are governed by the same field equation as in GR. The distinction lies in the interpretation of its constituent terms. In GR, the metric is postulated as a fundamental geometric field defined on a differentiable manifold, with curvature constructed intrinsically from that structure. In MQ, the metric

gμνsys
(I.63)

is a derived representation of the realized separation functional induced by the mapping. Curvature correspondingly arises from spatial variation of this separation functional.

The stress–energy tensor retains its operational role but differs in origin. In MQ it arises from variation of the matter contribution to the MQ Action, with matter content expressed through encoded availability and normalization under the Frames mapping. Geometry and source therefore originate from a common variational structure.

The gravitational coupling is likewise reinterpreted. In GR it is introduced empirically, whereas in MQ it follows from the dimensional structure of the fundamental measures and mapping-consistent scaling relations. The cosmological contribution is similarly derived from the MQ expansion structure rather than treated as a free phenomenological parameter.

These distinctions place MQ within the class of approaches in which gravitational dynamics emerge from a deeper substrate while preserving the empirical content of GR. In MQ, this substrate is explicitly kinematic and discrete, governed by conservation of count under the admissible Frames mapping.

An MQ description of expansion admits a homogeneous realization in which the separation functional defines a global background relation between System Frame and Internal Frame measures. This background fixes the normalization of expansion but does not determine local curvature, which remains governed by spatial variation of the realized separation functional.

gμνsys(x)=12∂2(nL+QL)2∂nμ∂nν.
(65)

In physical terms, this mapping-induced residual does not imply departure from spatial flatness of the homogeneous background realization. Rather, it introduces a normalization offset in the realized expansion rate while preserving the continuum geometric structure of the field equation. The MQ construction therefore predicts that a spatially flat background may coexist with a systematic mapping-induced offset in the realized expansion rate, providing a mapping-based interpretation of the Hubble tension [18].

Operationally, the homogeneous realization serves as a reference configuration fixing the relation between Internal Frame count evolution and System Frame expansion. Local gravitational dynamics arise from deviations from this background through spatial variation of the realized separation functional, ensuring that cosmological expansion and local curvature remain unified within a single separation functional while remaining dynamically distinct.

The significance of this formulation is twofold. First, the expansion scale follows from the same count structure that generates metric and curvature. Second, expansion normalization and local gravitational dynamics occupy distinct roles: the former fixes global normalization, while the latter governs local geometry.

4.3 Relation to prior unification efforts

The present construction is best understood in the context of prior unification programs seeking a common origin for gravitational and gauge structure. MQ shares with these approaches the objective of deriving gravitational dynamics from a deeper substrate while differing in both the nature of that substrate and the mechanism by which observable structure emerges through the Frames mapping.

Early unification efforts such as Kaluza–Klein theory [3] extend the dimensionality of spacetime, embedding gauge structure into a higher dimensional metric. In contrast, MQ introduces no additional dimensions. Instead, geometric and gauge related behavior arise from mapping-induced realization of count relations within a single kinematic domain.

Weyl’s unification program [4] similarly sought to incorporate electromagnetic structure into geometry through scale connection. In MQ, gauge behavior arises from normalization under the Frames mapping rather than from an independently postulated geometric connection.

Closer parallels exist with induced and emergent gravity approaches, in which the Einstein equation is treated as derived rather than fundamental. Sakharov’s induced gravity [5], Jacobson’s thermodynamic derivation [6], and related formulations [7,8] all treat gravitational dynamics as emergent. MQ aligns with this perspective in treating the field equation as derived but differs in that the underlying structure is neither statistical nor thermodynamic. It is kinematic and discrete, governed by the Frames Principle and conservation of count.

The distinction becomes explicit at the level of the action. In emergent approaches, one typically begins with an effective continuum action and interprets its origin through coarse-graining arguments. In MQ, the action is defined directly on the Internal Frame count domain, and continuum expressions appear only after normalization under the Frames mapping and coarse-graining. The Einstein–Hilbert and matter contributions are therefore interpreted as continuum representations of mapping-induced structure.

A further distinction lies in the treatment of scale. In higher dimensional and gauge-theoretic models, scale separation and coupling parameters are typically introduced independently. In MQ, scale dependence is governed by count separation within the Internal Frame, with distinct physical regimes arising from this dependence without introducing independent adjustable couplings.

The resulting position of MQ relative to prior work can therefore be stated succinctly: like geometric unification programs, it seeks a common origin for gravitational and gauge structure; like emergent-gravity approaches, it treats the Einstein equation as derived. It differs from both by locating this structure in a single discrete kinematic mapping between count and continuum representations.

4.4 Restricted uniqueness of admissible Frames mappings

The remaining question is whether the Frames mapping introduces hidden freedom. Within MQ, an admissible Frames mapping is not an arbitrary map from the Internal Frame to the System Frame. It must preserve conserved count, induce a normalized System Frame realization, support repeatable macroscopic records, and satisfy holonomy-free closure on all contractible reference cycles. A valid realization exists only on a referenceable universe domain U, where the mapping establishes the consistent reference relations required for observables. An admissible Frames mapping is therefore defined only on domains U satisfying the referenceability conditions given in Appx. A and developed through the realization structure of Appx. K.

Let M1 and M2 be two admissible Frames mappings on the same referenceable universe domain U. For every relational region ω'⊂U, each mapping realizes the same conserved Internal Frame count structure into its corresponding System Frame relational image,

Mi:ω'→Ωi(ω'), i = 1,2. (66)

For each admissible mapping Mi, the realized relational image is Ωi=Mi(ω')⊆R, where R is the System Frame realization structure. The images Ω1 and Ω2 do not denote physically distinct System Frames. They represent candidate realizations obtained from admissible Frames mappings prior to equivalence identification within the same realization structure R.

The realized separation functional is the mapping-normalized realization of conserved count,

RMi(ω')=NMi[C(ω')]
(I.64)

, i = 1,2, (67)

where C(ω') is the count functional fixed by conserved Internal Frame count and N[ω'] is the mapping normalization functional defined in Appx. A.3. Both are determined by count conservation, invariance under admissible relabelings, and the global normalization and holonomy constraints imposed by the Frames mapping. Admissibility excludes dependence on System Frame coordinates or non-conserved Internal Frame structure.

For any relational region ω', admissibility restricts normalization to a scalar action on the conserved count functional,

NMi[C(ω')]=λ(Mi)C(ω'),
(68)

where λ(Mi) is a mapping-dependent normalization factor fixed globally by the requirement of consistent boundary-flux realization and holonomy-free closure on all contractible cycles, and the scalar form is restricted to admissible configurations satisfying these constraints. This scalar form follows from the requirement that N preserve additivity over disjoint relational regions and invariance under admissible relabelings, as required by the definition of the count functional. No region-dependent or configuration-dependent modification is admissible, as such dependence would violate conservation or induce path-dependent realizations.

Since ω' is the same relational region in the same referenceable domain, conservation fixes C(ω'). Admissibility then requires equality of realized separations,

NM1[C(ω')]=NM2[C(ω')]∀ω'⊂U.
(69)

Substituting Eq. (68) into Eq. (69) yields λ(M1)=λ(M2). Thus, the normalization factor is uniquely fixed across all admissible Frames mappings on U. The normalization is therefore not free but determined by admissibility constraints on the domain.

The closure constraint follows from the requirement that realized observables be independent of reference path. Because the Frames mapping defines System Frame relations through coarse-grained realization of Internal Frame count, consistency requires that all contractible reference cycles produce no residual mismatch. For every contractible reference cycle γ⊂U, admissibility requires

HMi=0
(I.65)

, i = 1,2, ∀γ⊂U. (70)

This condition enforces path-independence of realized observables on contractible cycles and follows directly from the definition of a referenceable universe domain.

Repeatable realization requires that physically admissible Frames mappings produce stable observables under repeated evaluation of the same relational region. Let

OMi(ω')
(I.66)

denote the ordered realized data associated with ω', consisting of realized separation, contractible-cycle closure, and stable record state. For admissible Frames mappings on the same domain U,

OM1(ω')=OM2(ω')∀ω'⊂U.
(71)

This equation is the substantive uniqueness constraint. It states that admissible Frames mappings on the same referenceable domain produce identical realized observables for every relational region. Any remaining difference between M1 and M2 is therefore representational.

Define the realized equivalence relation induced by Mi as

ω'∼Miω″⇔OMi(ω')=OMi(ω″),∀ω',ω″⊂U.
(72)

Using Eq. (72), the two equivalence relations coincide,

∼M1=∼M2
(I.67)

. Therefore M1 and M2 induce the same quotient of relational regions into realized System Frame observables.

The induced map between admissible realizations is

Φ21:M1(ω')→M2(ω').
(73)

This map is well-defined on equivalence classes induced by realized observables. Because Φ21 preserves normalization, repeatable realization, and holonomy-free closure by Eqs. (68–70), it defines a frames automorphism. Hence M2=Φ21∘M1, with

NΦ21∘M1[C(ω')]=NM1[C(ω')]HΦ21∘M1(γ)=0,,
(74)

Equations (72–74) establish restricted uniqueness. On a fixed referenceable universe domain, admissible Frames mappings form a single physical equivalence class,

[M]U={Φ∘M|Φ∈Aut(U,M)}.
(75)

Every representative of [M]U produces the same realized separations, record states, metric, curvature tensors, stress–energy tensor, gravitational coupling, and scalar contribution governing expansion. These quantities therefore depend only on the equivalence class [M]U, not on the representative mapping.

This result removes the immediate concern that the field equation derivation depends on arbitrary mapping choice. The derivation depends only on the equivalence class [M]U, not on a particular representative M. The local gravitational construction is therefore unique up to frames automorphism.

The remaining question is whether locally equivalent representatives can assemble into globally inequivalent realizations due to non-contractible structure. Let {Uα} be an admissible cover of a referenceable universe domain U, with each Uα satisfying normalization, repeatable realization, and holonomy-free closure on contractible cycles. From the restricted uniqueness result above, any two admissible Frames mappings on each Uα differ only by a frames automorphism,

M2,α=Φα∘M1,α.
(76)

On overlaps Uα∩Uβ, admissibility requires the realized observables to agree. Therefore,

Φα∘M1=Φβ∘M1 on Uα∩Uβ, (77)

so the transition automorphism

Φαβ=Φβ-1∘Φα,
(78)


acts trivially on all realized observables in the overlap. This trivial action holds only at the level of realized observables and does not imply identity on the Internal Frame configuration domain.

Thus, for every contractible chain of overlaps,

ΦαβΦβγΦγα=id.
(79)

This cocycle condition ensures consistency of gluing across overlaps within the referenceable domain. It states that locally unique admissible Frames mappings assemble into a unique global equivalence class whenever no residual automorphism accumulates around contractible overlap cycles.

Nontrivial global freedom can arise only from non-contractible cycles or mapping defects. Let D denote the mapping defect class and let γ* denote a non-contractible reference cycle in U∖D. The only possible global invariant is defect holonomy,

HM(γ*)≠0γ*⊂U\D,.
(80)

Two globally admissible mappings are therefore physically equivalent if and only if they have the same realized local observables and the same defect-holonomy data,

M1∼M2⇔OM1(ω')→OM2(ω')∀ω'⊂U,
(81)
HM1(γ*)=HM2(γ*)∀γ*.
(82)

The equivalence is defined over all relational regions and all non-contractible reference cycles in U∖D. This yields the global classification result in restricted form: admissible Frames mappings on a referenceable universe domain are classified by their local automorphism class together with their non-contractible defect holonomy data,

[M]Uglobal=([M]U,D,{HM(γ*)}).
(83)

Since the local class [M]U is uniquely determined by observable and normalization constraints through Eqs. (71–75), any remaining inequivalence is entirely global and is exhausted by defect data. No additional invariant is introduced unless it corresponds to a distinct mapping defect class or non-contractible holonomy.

The mapping used in the field equation derivation is therefore not arbitrary. On each referenceable universe domain, admissible Frames mappings are locally unique up to frames automorphism and globally classified by non-contractible defect holonomy data. Accordingly, any remaining non-uniqueness belongs strictly to global topological structure and not to the construction of the Einstein field equation within MQ.

4.5 Falsifiability and scope

The derivation presented here is constrained by internal consistency conditions that follow directly from the Frames Principle and the MQ variational principle. These conditions define explicit operational failure modes at the level of realized observables and therefore establish the falsifiability of the construction.

A necessary requirement is that the realized separation functional admit a well-defined continuum limit under admissible coarse-graining. This limit must remain stable under admissible refinement and independent of coarse-graining choice within a fixed referenceable universe domain. The emergence of the differentiable metric structure

gμνsys
(I.68)

depends on the convergence and stability of this limit. Failure of convergence, or dependence on admissible coarse-graining choice, would invalidate the emergence of the metric and falsify the geometric construction.

A second requirement is that the mapping-induced variational structure produce a unique correspondence between deformation and gravitational coupling. Predictive determinacy requires that all admissible realizations consistent with the MQ variational principle yield the same gravitational coupling in the continuum limit on a fixed referenceable universe domain. Any residual freedom would imply that the coupling is not uniquely fixed by the underlying kinematic structure.

A third requirement is that conservation of count in the Internal Frame map to a conserved current in the System Frame without additional dynamical structure. The resulting continuity relation must arise solely from normalization under the Frames mapping and preserved count flux. Failure of conservation under admissible mapping would invalidate the derivation of realized conservation laws.

A fourth requirement is that the macroscopic field equation governing

gμνsys
(I.69)

be recovered without independent postulates beyond the MQ variational principle and admissible Frames mapping. The Einstein field equation derived in Sections 2–3 must emerge solely from the MQ variational principle and mapping structure in the continuum limit of admissible realizations. Dependence on externally imposed geometric identities or independently specified matter structure would invalidate the derivation.

These conditions define the internal falsifiability of the framework. Each condition constitutes an independent necessary requirement, and failure of any single condition produces a breakdown of the derivation. Their satisfaction establishes derivational closure.

In addition to these internal criteria, the present formulation has two scope limitations that bound its present completeness without affecting the field equation derivation.

First, admissible Frames mappings have been shown to be locally unique up to frames automorphism on any fixed referenceable universe domain, while global realizations remain classified by the mapping defect class and associated non-contractible holonomy data established in Section 4.4. The remaining open problem is therefore not local uniqueness but the exhaustive classification of globally inequivalent defect-bearing domains and their associated non-contractible holonomy classes. These global classes correspond to physically distinguishable realizations only insofar as their defect-holonomy structure induces observable differences in large-scale realized relational structure. They therefore provide a falsifiable aspect of the framework through possible observational signatures in global topology, large-scale anisotropy, or expansion structure. Such signatures, if present, would appear as departures from mapping-consistent predictions in large-scale angular correlations or distance–redshift structure.

Second, the present work derives the classical gravitational field equation in the continuum limit but does not provide a complete dynamical unification of relativistic and quantum field degrees of freedom within the MQ framework. In this context, “classical” refers to the continuum field equation governing the emergent metric

gμνsys
(I.70)

. A complete unification requires extension of the same mapping-consistent action structure to relativistic quantum dynamical degrees of freedom. Such extensions are necessary to establish full dynamical unification but lie beyond the scope of the present work.

APPENDICES

APPENDIX A: DEFINITIONS OF KEYWORDS, TERMS AND SYMBOLS

Notes

In earlier publications (prior to 2026), the roles of the Internal Frame and System Frame were described using a dimension-based distinction. With the formal identification of the Frames mapping, this characterization has been refined to align with the kinematic structure defined in the present work. The Internal Frame is now understood strictly as a discrete, count-based configuration domain without intrinsic geometric or continuous measure, while the System Frame represents the relational encoding in which observables are realized following application of the Frames mapping.

This refinement does not constitute a reversal of physical interpretation, but rather a clarification: geometry, continuity, and measurement arise only through the mapping from discrete count structure to relational observables. The realization of observables corresponds to the mapping-normalized encoding of conserved count, as defined by the mapping normalization functional. In this sense, normalization specifies the conditions under which Internal Frame configurations admit consistent, repeatable representation in the System Frame, and thereby defines the operational meaning of measurement.

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 any independent dynamical components.

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]=∫RL(ρR,∂ρR,…)dμ,
(I.71)

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 regime.

Curvature–resolved regime

A curvature–resolved regime 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

∂ρI(ξ,A)∂A+div⁡adjJI(ξ,A)
(I.72)

= 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

∂ρI(ξ,A)∂A+div⁡adjJI(ξ,A)=0
(I.73)

, or equivalently,

∂ρI(ξ,A)∂A+∑ξ'∈∂Ω(ξ)JI(ξ→ξ',A)=0
(I.74)

. 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

NI(ω',A)=∑ξ∈ω'nI(ξ,A)
(I.75)

(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

∑ξ∈ω'nI(ξ,A)
(I.76)

. The symbol ξis 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

div⁡adjJI(ξ,A):=∑ξ'∈∂Ω(ξ)JI(ξ→ξ',A)
(I.77)

, 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

∂ρI(ξ,A)∂A+div⁡adjJI(ξ,A)=0
(I.78)

. 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

∂ρI(ξ,A)∂A+div⁡adjJI(ξ,A)=0
(I.79)

. Equivalently,

∂ρI(ξ,A)∂A+∑ξ'∈∂Ω(ξ)JI(ξ→ξ',A)=0
(I.80)

. Unlike a continuum divergence, div⁡adj 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 div⁡adjJI 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

div⁡adjJI(ξ,A):=∑ξ'∈∂Ω(ξ)JI(ξ→ξ',A)
(I.81)

, 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' ,

ϕI(∂ω',A)=∑(ξ,ξ')∈∂ω'J(ξ→ξ',A)
(I.82)

, 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(r) — A System Frame observable function defined on the realized spatial coordinate domain r∈R3. The function f(r) represents an arbitrary measurable quantity evaluated on a realized configuration and is used to construct expectation values over the normalized encoded availability density ρP(r,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

⟨f⟩=∫R3f(r)ρP(r,t)d3r
(I.83)

, 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

N[ω']=1/Z(ω')withZ(ω')=∑ξ∈ω'nI(ξ,A)
(I.84)

. 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  ≡  ∇ln⁡ρR, 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,

ρR→ρR'=eχρR
(I.85)

, 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

nk(t)=∫AkρS(r,t)d3r
(I.86)

. Represents the pre–normalized encoded availability in region Ak. Used to construct conditional probabilities via normalization: P(k)=nk(t)/N1(t).

ρS(r,t) — System Frame encoded availability density

ρS(r,t)=dNSd3r=lim⁡ΔV→0nS(ΔV,t)ΔV
(I.87)

.
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(r,t) d3r. 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(r,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.

g(r,t) — System Frame log–gradient availability field (dimension 1/length), defined by

g(r,t)=∇ln⁡ρS(r,t)=∇ρS(r,t)ρS(r,t);
(U.6)

measures fractional spatial variation of encoded availability density.

r — is the System Frame spatial coordinate vector r∈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(r,t), P(r,t), J(r,t), v(r,t), Q(r,t), and ψ(r,t). Represents position within the realized three-dimensional spatial domain Ω. Distinct from the spacetime coordinate xμ 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

gμνsys
(I.88)

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

∇μVμ=1-gsys∂μ(-gsysVμ)
(I.89)

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

gμνsys
(I.90)

, connection coefficients

Γμνρ
(I.91)

, 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 r, 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

N1(t)=∫R3ρS(r,t)d3r
(I.92)

.

N2(t) — total encoded availability count in the bipartite (two–subsystem) System Frame normalization, defined by the inline equation

N2(t)=∫R3∫R3ρS(rA,rB,t)d3rAd3rB
(I.93)

.

ρP(r,t) — normalized System Frame probability density

ρP(r,t)=ρS(r,t)NS(t),∫ΩρP(r,t)d3r=1
(I.94)

. Dimensionless normalized probability density derived from the realized encoded availability density ρS(r,t). Defines realized outcome probabilities and detection statistics within the System Frame. The MQ wave function satisfies

ψMQ=ρPeiϕ,∣ΨMQ∣2=ρP
(I.95)

. 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(r,t),ρP2(r,t) — marginal probability densities for subsystems 1 and 2 obtained by integrating the joint density over the other subsystem’s 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=Oout
(I.96)

and 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
(I.97)

. Probabilities are obtained by normalization of encoded availability over these subsets, with outcome weights given by

nk(t)=∫Akρ(r,t)d3r
(I.98)

, 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.

χAk(r)
(I.99)

— is associated with each subset Akis the indicator function

χAk(r)
(I.100)

, defined by

χAk(r)=1
(I.101)

for r∈Ak and 0 otherwise, which implements restriction and conditioning of encoded availability and wave function support to the corresponding measurement region.

ψ(r,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(r,t)=ρP(r,t)eiϕ(r,t)=ρP(r,t)eiS(r,t)/ℏ.
(I.102)

∣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(r,t).

Ĥ
(I.103)

— System Frame Hamiltonian operator governing unitary Schrödinger evolution in the encoded continuum representation. For a non-relativistic encoded state,

Ĥ=-(ℏ2/2m)∇2+V(r,t)
(I.104)

. The operator

Ĥ
(I.105)

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(r,t) and generates Schrödinger-form evolution through

iℏ∂Ψ∂t=ĤΨ
(I.106)

. The operator represents redistribution dynamics of normalized encoded availability under closed evolution. Under the admissibility and boundary conditions,

Ĥ
(I.107)

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(r,t) — potential energy function in the System Frame Schrödinger equation; may include external fields and interactions as encoded in the continuum representation.

ϕ(r,t) — is the dimensionless System Frame phase field of the encoded wave function ψ(r,t). The phase determines interference structure and generates momentum and velocity fields through its spatial and temporal gradients.

S(r,t) — is the phase action field of the encoded wave function. S(r,t) carries units of action and is related to the dimensionless phase field by S(r,t)=ħ ϕ(r,t).

v(r,t) — is the System Frame velocity field in Madelung form, v(r,t)=(ℏ/m)∇ϕ(r,t)=(1/m)∇S(r,t).

p(r,t) — momentum field in the System Frame phase gradient representation, p(r,t)=ħ∇ϕ(r,t)=∇S(r,t), with p=m v when a velocity field is defined.

p̂
(I.108)

— momentum operator in position representation:

p̂=-iℏ∇
(I.109)

.

Jρ(r,t) — System Frame probability current density defined with respect to the normalized density ρp. It satisfies the continuity equation ∂tρp+∇⋅Jρ=0. In Madelung form,

Jρ=ρpv,v=ℏm∇ϕ.
(I.110)

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

∇2≈Δd(Δx)2
(I.111)

. 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(r,t) — quantum potential (Madelung form)

Q(r,t)=-ℏ22m∇2ρp(r,t)ρp(r,t)
(I.112)


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 [23] 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 [24] 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 [25]. 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 [26] 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 limit of the System Frame. 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— is the total density

ρtot=3Hsys2/8πG
(I.113)

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— is 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— is 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— is 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.

ρsys— is the MQ geometric density

ρsys=Λc2/2lf
(I.114)

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— is 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— is the baryonic matter fraction (ΛCDM comparison bookkeeping).

Ωc— is the cold dark matter fraction (ΛCDM comparison bookkeeping).

gμνsys
(I.115)

— denotes the emergent metric tensor in the realized System Frame. It defines the local continuum metric structure associated with mapped measurable separations under the Frames mapping. Unlike standard general relativity, where gμν is treated as a fundamental spacetime field, MQ treats

gμνsys
(I.116)

as a derived object obtained through coarse–graining of the realized separation functional. Its normalization is fixed by mapping constraints and is not independently specified.

Gμνsys
(I.117)

— denotes the Einstein tensor in the realized System Frame. It is constructed from the emergent metric tensor

gμνsys
(I.118)

through the associated Levi–Civita connection and resulting curvature contractions. In MQ,

Gμνsys
(I.119)

represents the continuum realization of higher-order discrete variation induced by the Frames mapping. Its divergence-free property follows from the metric-compatible connection and associated Bianchi identity, rather than from an independently postulated geometric structure.

Tμνsys
(I.120)

— denotes the stress–energy tensor in the realized System Frame. In MQ, it is defined variationally from the MQ Action through metric variation,

Tμνsys=-2-gsysδSmatterδgsysμν
(I.121)

, and therefore encodes the response of realized normalized count density to variations in the emergent metric structure. It is not independently specified and inherits its structure from encoded availability and mapping normalization.

Ksys — denotes the MQ gravitational coupling factor appearing in the realized field equation of the System Frame. It defines the proportional coupling between the realized curvature sector and the mapping-induced stress–energy structure. Unlike standard general relativity, Ksys is not introduced as an independent phenomenological constant, but is derived from the MQ primitive measures and the Frames mapping. In the realized continuum limit of the System Frame, Ksys=8πG/c4=4πtf/θsi. The quantity therefore encodes the mapping-normalized gravitational response implied by the conserved Internal Frame count structure under coarse-grained realization.

Λsys — denotes the realized cosmological term appearing in the System Frame 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 tensor

gμνsys
(I.122)

. 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 rather than introduced as an independent phenomenological parameter.

APPENDIX B: HOW TO DERIVE THE PLANCK EXPRESSIONS

Such that G=c3tf/mf ([9], Appx. F), ħ=2θsilf ([9], Appx. R) and the fundamental expression lfmf=2θsitf ([9], Appx. V), then

Length

lfmf=2θsitf,
(B.1)
lfmf=(2θsilf)GlfGtf=ℏGlfGtf,
(B.2)
lfmf(c3tfmf)=ℏGlftf,
(B.3)
lfc4tf=ℏG,
(B.4)
lf=(ℏGc3)1/2.
(B.5)

Time

lfcc=(ℏGc3)1/2,
(B.6)
tf=(ℏGc5)1/2.
(B.7)

Mass

tf=(ℏG2c5G)1/2,
(B.8)
tf=Gc3(ℏcG)1/2=c3tfmf1c3(ℏcG)1/2,
(B.9)
mf=(ℏcG)1/2.
(B.10)

Replacing the macroscopic measures of ħ and G with their corresponding electromagnetic measures, resolves Planck’s formulations.

lP=(ℏGc3)1/2.
(B.11)
tP=(ℏGc5)1/2.
(B.12)
mP=(ℏcG)1/2.
(B.13)

APPENDIX C: DISCRETE KINEMATICS AND THE MQ ACTION PRINCIPLE

MQ is defined on a discrete substrate consisting of the irreducible measures (lf, mf, tf) together with the dimensionless scaling parameter θsi, which fixes the relative weighting of count increments under admissible realizations. These quantities define the minimal count structure of the Internal Frame, from which all observable structure arises through the Frames mapping.

In this framework, admissible evolution is represented by ordered updates of count assignments rather than differentiable curves. No geometric or manifold structure is assumed at the primitive level. Geometry arises only through the mapping-normalized realization of conserved count in the System Frame.

The fundamental kinematic structure is defined by the discrete redistribution of count over the Internal Frame adjacency domain. Evolution proceeds through the update index A, with transport of count encoded by the adjacency flux Φ and governed by conservation relations expressed through the adjacency divergence operator divadj. This structure does not define a differential operator and does not act on a continuum domain. Its action is entirely combinatorial, defined within the discrete adjacency relations of the Internal Frame, and is subject to conservation, normalization, and admissibility constraints imposed by the Frames mapping.

Curvature is identified at the discrete level as the failure of successive admissible updates to commute. For a count-displacement object nγ, the discrete curvature operator is defined as the anti-symmetrized second-order adjacency redistribution of count over admissible update sequences,

R'(ω')=(divadjΦ)(2)(ω')-(divadjΦ)rev(2)(ω').
(C.1)

The non-commutativity expressed above does not arise from algebraic properties of finite differences alone, but from the admissibility constraints governing count transport. These constraints enforce conservation, normalization, and closure under the Frames mapping, and therefore restrict the allowed update sequences. The resulting obstruction to commutativity is a structural property of the discrete count dynamics.

The equation is also an Internal Frame analog of the standard curvature construction in which continuum curvature measures the non-commutativity of covariant transport. The analogy is structural only. In contrast to GR, no connection, metric, or differentiable manifold is defined at this stage. The quantity R'(ω') is therefore not a Riemann tensor, but a discrete obstruction to commuting admissible update sequences defined over the adjacency structure.

A continuum geometric representation arises only after coarse-graining over relational regions under the Frames mapping. The emergent metric and associated curvature tensors are constructed from the realized separation functional in Secs. 2.3–2.4. In that construction, the continuum curvature tensor is obtained from derivatives of the emergent metric, itself derived from the realized separation relation. The discrete obstruction defined above provides the primitive kinematic origin of this structure.

Thus, curvature in the System Frame is the continuum realization of second-order non-commutativity in admissible count transport. The geometric structure of relativistic physics arises as the unique coarse-grained representation of discrete kinematics governed by the MQ Action and the MQ variational principle.

APPENDIX D: FRAMES APPROACH TO THE HUBBLE TENSION

We describe the Hubble tension within the MQ framework as a consequence of the Frames mapping, building on the analysis presented in AIP Advances [18]. In this formulation, expansion measurements obtained from CMB observations and cepheid-based distance ladders are interpreted as frame-dependent realizations of a single underlying scalar expansion parameter. Specifically, measurements correspond to realizations in the System Frame and the Internal Frame, respectively, each arising from the same mapping-consistent scalar.

The distinction between these realizations is expressed through a mapping-induced normalization offset in the scalar expansion parameter θsi, which we denote as ΔH. This quantity reflects a shift in normalization under the Frames mapping and does not introduce an independent dynamical degree of freedom. The scalar difference is defined by

ΔH=θsi-π.
(D.1)

Following the construction in ([18], Eq. 61), the baseline scalar expansion parameter is defined by H=θsi, consistent with the scalar expansion parameter defined in Appx. A.5 and the expansion construction developed in Appx. G. Measurements obtained from CMB observations correspond to realizations in the non-discrete System Frame, while cepheid-based measurements correspond to realizations in the discrete Internal Frame. The respective frame-dependent expansion rates are therefore expressed as

Hsys=f(H-ΔH),
(D.2)
Hint=f(H+ΔH).
(D.3)

Here, the function f(⋅) denotes the mapping-consistent normalization that converts the dimensionless scalar expansion parameter into an observable quantity. It is not an arbitrary functional degree of freedom but is fixed by the normalization procedure defined through the Frames mapping.

Substituting H = θsi and ∆H = θsi-π, we obtain

Hsys=f(H-ΔH)=f(θsi-(θsi-π))=f(π).
(D.4)

This demonstrates that the System Frame realization depends only on the invariant value π. Combining the above relations yields a closed expression for the Internal Frame realization,

Hint-f(ΔH)=Hsys+f(ΔH),
(D.5)
Hint=Hsys+f(2ΔH)=f(π)+f(2θsi-2π)=f(2θsi-π).
(D.6)

To connect these scalar expressions to observational quantities, we now resolve the baseline expansion rate in standard cosmological units. The scalar quantity H is dimensionless in the MQ construction (Appx. A.5), and physical units arise only through mapping-consistent normalization. The scalar H retains its definition as a dimensionless quantity. Normalization introduces only its representation in physical units and does not redefine the underlying parameter. Expressing H in mapping-normalized units, we define

H=1AUkmMpc
(I.123)

, with

AU=DU2θsi
(I.124)

(D.7)

we obtain

H=1AUkmMpc=2θsiDUkmMpc.
(D.8)

This step makes explicit that the conventional units of the Hubble parameter arise from the mapping between the dimensionless scalar expansion rate and the System Frame distance normalization. No additional dimensional constants are introduced. The units follow directly from the definition of the observable separation scale.

We may now evaluate the frame-dependent expressions by substituting π or 2θsi-π into the normalized form. The resulting values are

Hsys=πθsiAUkm/Mpcs/y109=68.261kms-1Mpc-1,
(D.9)
Hint=(2θsi-π)θsiAUkm/Mpcs/y109=73.510kms-1Mpc-1.
(D.10)

These values reproduce the observed separation between CMB inferred and cepheid inferred measurements of the Hubble constant, yielding a 3.35σ right-tail concordance with the SPT-3G observations [16], the Pantheon+ cosmological constraints [17], and the MQ Hubble tension analysis [18] (Appx. H). While individual experimental determinations vary across collaborations, the present construction captures the characteristic scale of the discrepancy without introducing additional parameters. The difference therefore emerges as a direct consequence of the mapping-consistent distinction between System Frame and Internal Frame realizations.

We emphasize that θsi carries no units when treated as a scalar expansion parameter in the System Frame (Appx. A.5), and that all physical units associated with H arise from the normalization procedure described above. The resulting expressions are therefore dimensionally complete and consistent with standard cosmological measurements.

APPENDIX E: COSMOLOGICAL TERM AS AN MQ CALCULATED VALUE

Using the standard FRW relation between the cosmological constant and the dark energy density parameter,

ΩΛ=ρΛρc=Λc2/(8πG)3H02/(8πG)=Λc23H02,
(E.1)

we may express Λ in terms of the scalar fraction and the dimensionful expansion rate. In the MQ construction this gives

Λsys=3ΩΛH02c2,
(E.2)

where ΩΛ is understood as the scalar fraction in the standard cosmological parametrization. Within MQ, this fraction is not independently specified but arises directly from mapping consistent normalization of the expansion structure. The corresponding MQ expression follows from the mapping consistent scalar fraction derived in Appx. G,

Ωdk=θsi2-2θsi2+2,
(E.3)

where θsi is the mapping-defined scalar that sets the relative scaling of count increments and fixes the global expansion normalization. The discrete–to–continuum normalization is realized through the count-to-coordinate mapping and the associated coarse-grained metric construction (Eqs. 17–21). This quantity replaces ΩΛ in the MQ construction and is determined entirely by invariant internal relations under the Frames mapping.

We insert the MQ expansion rates for the Internal Frame and System Frame realizations ([18], Eqs. 84–85),

Hsys=πθsiAU(km/Mpcs/y109),
(E.4)
Hint=(2θsi-π)θsiAU(km/Mpcs/y109),
(E.5)

which represents mapping-normalized realizations of the scalar expansion parameter. Using Λ=3ΩdkH2/c2 for each frame yields

Λsys=3ΩΛHsys2c2,
(E.6)
Λint=3ΩΛHint2c2.
(E.7)

Substituting the mapping-defined scalar fraction and expansion rates gives the dimensionless geometric coefficients

Λsyslf2=3θsi2-2θsi2+2(πθsicAUkm/Mpcs/y109)2=2.9167928(11)×10-122,
(E.8)
Λintlf2=3θsi2-2θsi2+2((2θsi-π)θsicAUkm/Mpcs/y109)23.38266(19)×10-122.
(E.9)

These values depend only on mapping normalization through AU and the invariant scalar θsi and therefore reflect the MQ geometric structure rather than an independently specified cosmological constant.

For comparison with the GR interpretation, the corresponding vacuum energy density is

ρvac=Λc28πG,
(E.10)

which expresses the standard continuum relation between Λ and vacuum energy.

Within MQ, a geometric density may be constructed directly from the mapping-defined scalar without invoking the GR definition. Using

ρvacframe=Λframec2/2lf
(I.125)

, the frame-resolved densities are

ρvacint=5.6899(16)×10-27kgm-3,
(E.11)
ρvacsys=5.2835731(11)×10-27kgm-3.
(E.12)

These correspond to cosmological constants of 1.29500 × 10–52 m2 (Internal Frame) and 1.11665 × 10–52 m2 (System Frame). Within uncertainties, the System Frame value is consistent with the cosmological constant inferred from the Planck 2018 parameter set, ΛCMB = 1.11(02) × 10-52 m-2 [27], yielding a 4.50σ right-tail concordance.

The GR relation in Eq. (E.10) provides an interpretive mapping to standard cosmology, whereas Eqs. (E.11–E.12) give the MQ geometric density derived directly from mapping-realized count structure.

The continuum curvature entering the MQ field equation is constructed from the emergent metric

gμνsys
(I.126)

, whose form is fixed by the realized separation functional (Eqs. 17–21). The mapping from discrete count structure to continuum geometry is therefore uniquely determined by the same functional that defines realized separation.

In this construction, curvature in the System Frame is not introduced independently but arises as the continuum representation of the underlying count structure under the Frames mapping. The metric, connection, and curvature thus form a closed construction without additional postulates beyond those defining realized separation.

APPENDIX F: FRAME–DEPENDENT DIMENSIONAL ANALYSIS IN MQ

In the Internal Frame, θsi is treated as a dimensionless structural quantity associated with the count-based configuration underlying realization. Its numerical value is invariant and equal to the same fundamental quantity that appears throughout MQ, θsi=3.262390305….

The absence of physical dimensions in the Internal Frame does not alter the numerical value of θsi. Rather, it reflects that count relations are defined prior to realization and therefore do not yet possess units of length, mass, time, or momentum. Dimensional quantities emerge only after application of the Frames mapping, which converts count-based structure into realized observables in the System Frame.

Under realization through the fundamental measures (lf, mf, tf), the same structural quantity acquires the dimensions of momentum,

θsys=lfmf2tf,
(F.1)

while retaining the identical numerical value. The distinction between θint and θsys is therefore not one of magnitude but of representation. In the Internal Frame, θsi is dimensionless because it is expressed as a normalized count-based structural quantity. In the System Frame, the same quantity is realized through the fundamental measures and therefore carries the dimensions of momentum.

By contrast, the System Frame realization θsys, numerically identical to θsi which is used throughout MQ, is dimensionful and corresponds to half of the fundamental momentum under realization through (lf, mf, tf). Internal Frame quantities specify count relations. Physical dimensions enter only when those relations are realized through (lf, mf, tf) in the System Frame. A dimensionless representation arises only when the same structure is expressed as a normalized ratio under the discrete–continuous mapping, as demonstrated by the Unity Expression ([9], Appx. AX),

(12θsi)2/3+(nLnLc)2=1.
(F.2)

Thus, the frame of reference must always be considered when carrying out a unit analysis. A second consideration arises from substitutions involving θsi = lfmf/2tf, where mixing structural and realized forms can introduce spurious dimensional factors. Consider, for example, its use as a scalar relating the age of the universe to its diameter, DU = 2θsiAU. θsi serves as a scalar, yet the substitution formally introduces the relation L/T → ML/T. Without careful interpretation, such substitutions can incorrectly introduce mass dimensions into purely kinematic relations. The most notable examples occur in descriptions of the Hubble constant and related universe-scale normalization relations (Appx. G).

Hsys=πθsiAU(km/Mpcs/y109).
(F.3)

In reducing expressions similar to the Hubble constant one may replace AU = DU/2θsi. This changes the units from seconds to seconds per kilogram, 1/(LM/T)T = 1/LM. This apparent inconsistency reflects the improper treatment of θsi as a dimensional quantity rather than a mapping-normalized scalar.

In our description of the cosmological constant, we find the first instance applies:

Λsys=3(πθsiAUckm/Mpcs/y109)2θsi2-2θsi2+2.
(F.4)

In this example we can focus on the denominator. That is, (LM/T)T(L/T) = L²M/T. However, because θsi enters as a System Frame scalar, its apparent units are not applicable and θsi should be treated as dimensionless. Therein, we recognize that this expression should have been written as T(L/T) = 1/L, giving us length squared in the numerator when considering the ratio is in parenthesis squared. With this correction, the expression yields the expected dimensional form for the cosmological constant, Λ ∼ L⁻².

With regard to nomenclature, it is sometimes necessary to suppress the explicit subscript “si” when clarifying labels such as “int” and “sys” are needed. MQ imposes no rigid rule for which frame labels take priority. The choice is made to prevent ambiguity in the surrounding expressions.

Historically, the subscript “si” has been typeset in italics. While we preserve that convention here, italics can occasionally obscure meaning when θsi appears inside field equations. Future presentations may prefer a non-italic subscript for clarity.

It is also important to clarify the origin of the “si” designation. The value of θₛᵢ arises from experimental measurements of entangled X-ray signal–idler pairs at their degenerate frequency, as reported by Shwartz and Harris [28,29]. Its interpretation within the MQ framework is developed in Ref. [9].

In a specific configuration, the signal and idler polarization angles are equal. Their measured value, θₛᵢ ≈ 3.26239 radians, corresponds directly to half of the fundamental momentum. This identification is made explicit in Ref. [9], Appx. A, where the signal, idler, and pump angles are expressed within the MQ formalism. It is further developed in Ref. [9], Appx. S, where the fundamental expression – a parallel construct to the Planck units that includes non-Lorentz length contraction – demonstrates that angular measure and momentum are equal in value and physically correlated at the bound.

Thus, θₛᵢ represents a measured physical quantity whose angular and momentum representations are dual descriptions of the same underlying structure. Whether θₛᵢ is dimensionless or dimensionful depends on how the relation is expressed. When represented as a normalized mapping in the Internal Frame, it is dimensionless. When realized through (lf, mf, tf) in the System Frame, it becomes dimensionful.

Failure to distinguish between these two roles leads to incorrect dimensional interpretations within MQ.

APPENDIX G: PHYSICALLY SIGNIFICANT DOMAINS OF THE OBSERVABLE UNIVERSE

Definitions

Ωtot=Ωobs+Ωdk.
(G.1)
Ωdk+Ωobs=1.
(G.2)
Ωobs=2θsiΩvis.
(G.3)
Ωuobs=Ωobs-Ωvis.
(G.4)

Calculations

2θsiΩvis=Ωobs,
(G.5)
2θsi2=4ΩvisθsiΩobs=Ωf,
(G.6)
Ωf=2θsi2.
(G.7)
2θsiΩvis=Ωobs,
(G.8)
2θsiΩvisθsi22-1=Ωobsθsi22-1,
(G.9)
θsi3Ωvis-1=Ωobsθsi22-1.
(G.10)

Given the dark equality above and such that Ωdk+Ωobs=Ωtot , then we replace the Ωobs to show that,

Ωdk=(Ωtot-Ωdk)θsi22-1=(1-Ωdk)θsi22-1.
(G.11)
Ωdk=(1-Ωdk)θsi22-1.
(G.12)
Ωdk=θsi2-2θsi2+2.
(G.13)

Such that the dark is the total (i.e., 1) minus the observable, then

1-Ωobs=Ωobsθsi22-1.
(G.14)
2=Ωobsθsi22+Ωobs,
(G.15)
Ωobs=4θsi2+2.
(G.16)
Ωobs=2θsiΩvis=4θsi2+2,
(G.17)
Ωvis=2θsi(θsi2+2).
(G.18)
Ωuobs=Ωobs-Ωvis=4θsi-2θsi(θsi2+2).
(G.19)

APPENDIX H: CONCORDANCE ANALYSIS

Table II: Right tail p–value with Corresponding Agreement Sigma for 11 Implementations of the Frames Principle (2022 CODATA)*

Phenomenon

Exp.

Calculation

Measure

MQ Calculated

Measure

p–value

Pull

σagree

w/oMQ

G=QLrc3/θsi
(T.1)
Gravitational Constant (CODATA 2010) m3 kg−1 s−2

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

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

 

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

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

Global Concordance

 

 

 

 

 

0.9999

3.70

0.00

Hsys=(2π/2θsiAU)(km/Mpc / s/y 109)
(T.2)
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

αmea0kBhcTCMB

HCMB

68.259(19)

68.3(15)

0.978

2.74 10–2

2.02

n/a

Hint=(2(2θsi−π)/2θsiAU)(km/Mpc / s/y 109)
(T.3)
Hubble Constant (Pantheon+) km s–1 Mpc–1

αmea0kBhcTCMB

Hcepheids

73.508(21)

73.5(11)

0.994

7.47 10–3

2.51

n/a

2QLnLr(84θsi−⌊42θsi⌋)
(T.4)
Global Concordance

 

 

0.9996

2.84 10–2

3.35

n/a

Fine Structure Constant (Classical)

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

θsi=(ħc3/4G)1/2lfmf/2tf
(T.5)
 

αmea0c

ħGc

3.262 390 305(89)

3.262 390(23)

0.9999999997

3.45 10–10

6.20

4.79

Reduced Planck Constant J s

lfθsi/QLnLr
(T.6)
 

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

Magnetic Constant N A–2

2πγmf/c4lf
(T.7)
 

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

G=2πγ/μ0c2
(T.8)
Gravitational Constant – unification f(μ0) m3 kg−1 s−2

αμ0c

G

6.674 077 93(33) 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

(tf/2QLnLrαme)(ħc3/G)1/2
(T.9)
Bohr Radius (gravitational) m

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

4πε0ℏ2/mee2
(T.10)
Bohr Radius (electromagnetic) m

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

Global Concordance

0.99999996

2.74 10–4

5.38

0.00

MQ Tension Solutions (G, H0)

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 Frames Principle (Includes all 11 implementations)

 

 

 

 

 

1–(1.1 10–19)

4.56 10–2

8.74

0.00

* Gray text indicates implementations not included in the Frames Principle assessment.


The MQ concordance framework evaluates agreement between prediction and experiment through a statistically traceable methodology based on one-tailed χ² right-tail tests. Under the assumption that MQ is correct, the associated p-values represent the probability of obtaining discrepancies equal to or larger than those observed. Statistical agreement is expressed through σ = Φ⁻¹(p), while the pull statistic measures signed deviation relative to experimental uncertainty. Values with |pull| ≥ 2 are treated as potential indicators of disagreement. To ensure valid significance estimates, only physically independent observables contribute to the degrees of freedom, preventing duplication of common systematic effects. All calculated values originate from experimentally measured inputs using standard NIST uncertainty procedures, maintaining direct traceability between the “Calculation” and “Measure” columns. Throughout the analysis, MQ-corrected expressions are distinguished from classical (w/o MQ) formulations. Eliminating the discrete frame length contraction contribution, 2QLnL, recovers the corresponding Planck-based composite expressions and establishes the reference case used for comparison.

The concordance procedure is guided by the Frames Principle, which requires comparisons to be restricted to independent physical realizations of invariant couplings. Accordingly, CODATA quantities derived from common Planck relationships are not counted as independent confirmations. Instead, electromagnetic and macroscopic gravitational realizations are treated as separate experimental tests of the same underlying invariant structure. Parameters that lack direct measurement, such as θsi and, in some applications, ħ, are evaluated as derived quantities with uncertainties propagated from experimentally constrained inputs. A clear distinction is maintained between electromagnetic-scale evaluations and macroscopic-scale evaluations. MQ further requires a common evaluation distance, typically chosen at the upper interaction limit, thereby avoiding systematic offsets introduced by distance-dependent length contraction. The analysis is fully consistent with the modern SI system, where uncertainties in electromagnetic constants propagate through α. Consequently, derived quantities including a0, G, and α are evaluated within a common uncertainty framework that preserves internal consistency while providing a test of cross-domain unification.

STATEMENTS TATEMENTS 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

No datasets were generated or analyzed during the current study.

FUNDING

This research has received no external funding.

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