Properties of atoms. Discrete geometry in Measurement Quantization. Conceptual atomic illustration, not to scale. The bright curve is not a measured electron trajectory; the Bohr radius is a reference length rather than a universal atomic diameter or radius.

Properties of atoms

Discrete geometry in Measurement Quantization. MQ links atomic reference quantities through discrete counts, the dimensionless coefficient theta subscript si and fundamental measures. Observable quantities belong to the System Frame realization of Internal Frame structure under the Frames mapping. The displayed relations share calibration inputs; they are not three independent predictions of all atomic properties.

Bohr reference length

a subscript zero denotes the conventional Bohr reference length, in metres. m subscript f is the MQ fundamental mass in kilograms, m subscript e is electron mass in kilograms, l subscript f is the fundamental length in metres, and alpha subscript p is the dimensionless Planck-like fine-structure coupling used in this MQ realization.

a0=mfαpmelf

This exact rearrangement follows MQKB523 MQ2028 and MQ0346: fundamental length equals electron mass times Bohr radius times alpha subscript p divided by fundamental mass. The supplied infographic had the two mass factors reversed. The corrected numerator is fundamental mass, and the denominator contains electron mass. This input-chain relation does not independently determine the Bohr radius when calibrated using atomic data. CLM3541 identifies the Bohr radius as a conventional atomic reference scale, not a universal ground-state orbital radius for every atom. The illustration’s diameter-style annotation has therefore been removed.

Classical fine-structure coupling

Alpha subscript c is the dimensionless classical fine-structure coupling. n subscript L is the dimensionless separation or demarcation count parameter in the stated realization, and Q subscript L is its positive fractional residual. The product 2 Q subscript L n subscript L is dimensionless. Theta subscript si is dimensionless and distinct from its dimensional momentum realization, which is not used in these displayed equations.

αc−1=2QLnL(84θsi−⌊42θsi⌉)

MQ0066, MQ0070 and MQ2215 support the relation. The mixed left-floor and right-ceiling brackets denote rounding to the nearest integer, not ordinary floor or ceiling separately. Under the adopted branch, their argument is not at a half-integer tie. The source’s Planck-like inverse coupling is eighty-four theta subscript si minus that rounded integer; its distinction from the classical coupling is retained. These relations are used within a calibration construction and are not by themselves independent evidence for the entire framework.

Charge realizations

e subscript c is the classical elementary-charge realization and e subscript p is its Planck-like counterpart, both in coulombs.

ec=2QLnLep

This is MQ2083, also retained in MQ0195, MQ2200 and MQ2314. It presents the shared finite-count relation without the auxiliary r subscript q41 and fundamental-charge chain used in the historical expression. The simplified current form does not assume the historical gamma approximation. Any numerical charge prediction requires the source’s stated input and normalization conventions; no independent charge measurement or new numerical value is asserted here.

Illustration and sources

The atomic picture is an edited conceptual illustration, not a wavefunction, measured orbital, electron trajectory, nuclear composition determination or scaled atom. The cleaned artwork removes the original dimension arrow and flattened text while preserving its visual style. Source consistency is checked against MQKB523.zip. The conventional Bohr-radius definition is also documented in the CODATA 2022 primary tables at https://physics.nist.gov/cuu/pdf/wallet_2022.pdf . No numerical conventional constants or uncertainties were introduced in this infographic.

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Properties of Atoms

Atoms provide an especially useful setting in which to examine what changes when continuous physical expressions are reconstructed within Measurement Quantization. Conventional physics describes quantities such as elementary charge, the fine-structure constant, electron mass, and the Bohr radius through experimentally established relations and measured or defined constants. MQ does not replace those empirical descriptions. Instead, it asks whether the same quantities can be expressed through discrete counts, fundamental measures, and the mapping by which count relations are physically realized.

This distinction begins with the MQ treatment of frames of reference. The Internal Frame contains the discrete count relations underlying physical measure. These relations are realized through the Frames mapping in the System Frame, where dimensional quantities become physically observable. The distinction is therefore not simply between an observer and an observed object. It distinguishes the discrete relational description of measure from its continuous physical realization.

The relationship between these frames is central to the MQ description of atomic properties. A quantity can have an Internal Frame representation and a corresponding System Frame realization. When an underlying continuous relation does not coincide exactly with an admissible whole count, the resulting difference is retained by MQ as a Diophantine realization residual. The subsequent mapping of discrete count structure into a continuous observable also introduces the metric differential. At finite count separation, the associated geometric normalization is expressed through the Informativity differential.

The Fine-Structure Constant

The fine-structure constant α is a dimensionless physical constant characterizing the strength of electromagnetic interaction. In MQ, its inverse is especially useful because the fine-structure construction can be followed from a native Internal Frame expression through successive System Frame realizations. The native relation is αf−1=42θsi, where αf−1 is the fundamental inverse fine-structure quantity and θsi is the invariant MQ scalar. The factor 42 is established in the MQ construction from one-half of the electromagnetic interaction count rather than inferred from the target fine-structure value at this stage.

Because 42θsi does not coincide exactly with a whole count, MQ retains the residual Qnθ=42θsi−42θsi. The mixed floor-ceiling operator denotes realization to the nearest admissible whole count and replaces the explicit rounding notation used in earlier MQ treatments. Adding this residual gives the Planck-like System Frame quantity αp−1=84θsi−42θsi.

The Planck-like form is not yet the classically realized fine-structure constant. At the electromagnetic demarcation, the interaction-length count is nL=276θsi. The corresponding residual product is QLnL=nL1+nL2−nL, where QL is the finite-count residual associated with that count. The Internal Frame to System Frame differential is Δint−sys=αp−11−2QLnL.

Applying this finite-count correction produces the principal classically realized relation:

αc−1 = 2QLnL 84θsi − 42θsi

The two corrections have distinct roles. The whole-count residual transforms the native Internal Frame expression into its Planck-like realization. The finite-count normalization associated with the Informativity differential then maps that realization to the continuously expressed inverse fine-structure quantity observed in the System Frame.

What This Agreement Establishes

MQ can run the fine-structure construction in either direction. In the inverse determination used to establish the precision value of θsi, the measured classical inverse fine-structure constant is an experimental input, giving θsi=3.262390305(36). Reconstructing the fine-structure constant from that same precision value is therefore an internal closure calculation rather than an independent prediction of α. Its importance is structural. Once the scalar is fixed, the same count geometry and realization rules can be propagated into other MQ relations without introducing a new scalar for each phenomenon.

Elementary Charge

Elementary charge provides a dimensional application of the same realization structure. In the International System of Units, the elementary charge e is defined exactly as 1.602176634×10−19C. MQ distinguishes this SI-defined observable from three successive representations used in its derivation: the fundamental charge ef, the Planck-like charge ep, and the classically realized charge ec.

The fundamental charge is ef=lfθsi2mf2θsi−1, where lf and mf are the fundamental length and mass measures. Using the MQ fundamental relations, this is equivalently ef=lfc24θsi−1, yielding ef=1.60512538253(81)×10−19C.

This is the fundamental representation rather than the observable elementary charge. MQ next applies the charge-count realization ratio rq41. It is defined by rq41=nθ−1θsinθ−1θsi, where nθ is the applicable charge-count parameter. Its value is rq41=0.998197579719(51), giving ep=rq41ef=1.60223227199(59)×10−19C.

The remaining finite-count correction applies the same normalization factor encountered in the fine-structure construction. The classically realized charge is the principal result:

ec = 2QLnLep = 2QLnLrq41ef

The resulting MQ classical realization is ec=1.6021763105(70)×10−19C. This value is not an independent measurement of elementary charge. It is the classically realized value produced by the MQ construction. Comparison with the exact SI value tests the numerical closure of that construction subject to the inputs and dependencies used to establish its parameters.

What Charge Quantization Means Here

The MQ construction does not reduce to the statement that electric charge simply “must be a whole number.” It distinguishes an underlying fundamental quantity from its discrete realization and its subsequent finite-count normalization in the System Frame. This description does not require conventional quark charge assignments to be discarded. In particle physics, up-type quarks carry charge +2/3 e and down-type quarks carry −1/3 e. MQ's construction instead concerns realization of the electromagnetic charge scale.

Atomic Scale

The connection to atomic structure follows through the Bohr radius a0, the atomic unit of length associated with the characteristic ground-state scale of hydrogen. Within MQ, the fundamental length is related to electron mass me, the Bohr radius, the Planck-like fine-structure quantity αp, and fundamental mass mf.

lf = mea0αp mf

The MQ realization gives lf=1.616199912(18)×10−35m. The atomic scale is therefore connected to the same fundamental-measure system used in the electromagnetic construction. MQ records the dependence compactly as a0=fθsi, where f denotes the established functional dependence rather than a new independent physical parameter.

Atomic Spectra as a Consistency Constraint

If θsi varied during the expansionary history of the universe, that variation would propagate through the MQ measure relations and alter quantities tied to atomic structure. Changes affecting atomic energy levels would in turn be reflected in spectral transitions. Within MQ, distant atomic spectra therefore provide a consistency constraint on variation of the scalar. This is a constraint on the construction rather than independent proof of the framework.

A Common Realization Structure

The significance of the atomic construction is that the fine-structure constant, elementary charge, and atomic length scale are not treated as isolated numerical coincidences. They are connected through the same θsi, fundamental measures, count relations, and Frames mapping. The same framework is subsequently carried into gravitational quantities, including the gravitational constant.

This common dependence also determines how agreement should be interpreted. When a measured quantity is used upstream to determine an MQ parameter and is then reconstructed from that parameter, the result is an internal consistency or closure test. It is not an independent prediction. Stronger empirical tests arise when the established MQ structure is carried into observables that were not used to determine the parameters entering the calculation.

The properties of atoms therefore occupy an important position in Measurement Quantization. They connect experimentally established electromagnetic and atomic quantities to the discrete realization structure proposed by MQ. The central question is not whether conventional atomic physics should be replaced. It is whether the observed quantities can also be represented consistently as System Frame realizations of conserved count relations in the Internal Frame, and whether that same realization structure continues to hold when applied to independently measured phenomena.

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