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C3 × Z2 Interference Geometryand a Light-Fermion Mass Cascade
Andrew M. Brilliant
Posted: 28 May 2026
Towards Deriving the Standard Model Coupled to Gravity from Generalized Trace Dynamics via the Spectral Action Principle
Tejinder P. Singh
Posted: 26 May 2026
Stratification Criteria for Machine Learning Pattern Discovery in Particle Physics - Preparing for the AlphaFold Moment
Andrew Michael Brilliant
Posted: 25 May 2026
A Monte Carlo Null-Model Test of an Outer-Soddy Completion of the Koide Lepton Triple
Andrew M. Brilliant
The Koide relation \( Q = (\sum m_\ell)/(\sum \sqrt{m_\ell})^2 = 2/3 \) for the charged leptons has held to one part in \( 10^5 \) for over forty years without an accepted derivation and is widely regarded as numerology. This paper takes the relation as a clue rather than an endpoint. Treating lepton mass square roots as Descartes-circle curvatures, the outer root of the Descartes quadratic equals the closed form \( \mathcal{F} = e_1 - \sqrt{p_2} \) when Koide holds exactly (Proposition 1); equivalently, \( \mathcal{F}^2 = \alpha_K^2\,\mu_\star \) with \( \alpha_K^2 = 5/2 - \sqrt{6} \) and \( \mu_\star = \sum_\ell m_\ell \) the lepton-sum scale. The three-input symmetric-polynomial identity thus collapses to one dimensionless Koide-determined constant times the lepton-sum scale. Kocik [10] first observed a Descartes-like reading of Koide; our mutually-tangent variant is mathematically distinct but follows the same geometric spirit. The four-curvature completion carries a testable consequence absent from the bare three-mass relation: evaluating the squared fourth curvature numerically, \( \mathcal{F}^2 = 95.113 \) MeV, and comparing against the strange-quark \( \bar{MS} \) mass at \( \mu_\star \) within current lattice precision yields a residual of \( +0.04 \) MeV against \( \pm 0.69 \) MeV, about \( +0.06\sigma \). The lepton-side quantity is fixed to better than \( 0.01\% \); future lattice improvements will sharpen or refute the present numerical agreement. To our knowledge this paper implements the first Monte Carlo null test of the Koide relation under a random-spectrum prior; a Koide-conditioned null-model calibration across four prior shapes pre-registered for the analysis gives hit fractions at the sub-percent level — model-conditional frequencies, not \( p \)-values. Scale, input, prior, and filter sensitivities, together with the error budget, are reported; full Monte Carlo protocols, numerical output, and pre-registration are in a companion methods note [15].
The Koide relation \( Q = (\sum m_\ell)/(\sum \sqrt{m_\ell})^2 = 2/3 \) for the charged leptons has held to one part in \( 10^5 \) for over forty years without an accepted derivation and is widely regarded as numerology. This paper takes the relation as a clue rather than an endpoint. Treating lepton mass square roots as Descartes-circle curvatures, the outer root of the Descartes quadratic equals the closed form \( \mathcal{F} = e_1 - \sqrt{p_2} \) when Koide holds exactly (Proposition 1); equivalently, \( \mathcal{F}^2 = \alpha_K^2\,\mu_\star \) with \( \alpha_K^2 = 5/2 - \sqrt{6} \) and \( \mu_\star = \sum_\ell m_\ell \) the lepton-sum scale. The three-input symmetric-polynomial identity thus collapses to one dimensionless Koide-determined constant times the lepton-sum scale. Kocik [10] first observed a Descartes-like reading of Koide; our mutually-tangent variant is mathematically distinct but follows the same geometric spirit. The four-curvature completion carries a testable consequence absent from the bare three-mass relation: evaluating the squared fourth curvature numerically, \( \mathcal{F}^2 = 95.113 \) MeV, and comparing against the strange-quark \( \bar{MS} \) mass at \( \mu_\star \) within current lattice precision yields a residual of \( +0.04 \) MeV against \( \pm 0.69 \) MeV, about \( +0.06\sigma \). The lepton-side quantity is fixed to better than \( 0.01\% \); future lattice improvements will sharpen or refute the present numerical agreement. To our knowledge this paper implements the first Monte Carlo null test of the Koide relation under a random-spectrum prior; a Koide-conditioned null-model calibration across four prior shapes pre-registered for the analysis gives hit fractions at the sub-percent level — model-conditional frequencies, not \( p \)-values. Scale, input, prior, and filter sensitivities, together with the error budget, are reported; full Monte Carlo protocols, numerical output, and pre-registration are in a companion methods note [15].
Posted: 22 May 2026
Planck Scale Informational Physical Model and Fundamental Problems in Physics
Sergey V. Shevchenko
,Vladimir V. Tokarevsky
Posted: 22 May 2026
A Model for the Higgs Field
Tongsheng Xia
Posted: 06 May 2026
A Version of Exclusively Perturbative Quantum Field Theory
Sergey Larin
Posted: 22 April 2026
The Complex Hopf Fibration as the Canonical Space for Gauge–Gravity Unification: The Field, Universal Action, and Particle Spectrum
Jennifer Lorraine Nielsen
Posted: 20 April 2026
QICT Resolution of the Gauge-Hierarchy Problem: Information-Protected Mass Generation from Strictly Local Quantum Dynamics
Mohamed Sacha
Posted: 15 April 2026
Gyromagnetic Ratio of Electrically Neutral Particles: Case of the Neutron
Golden Gadzirayi Nyambuya
Posted: 14 April 2026
Discrete Time Quantum Walk in a QCD Chiral Condensate Lattice
Rami Rom
Posted: 14 April 2026
A New Way to Unify All Fermion and Boson Fields, Including Gravity
N. S. Mankoč Borštnik
Posted: 13 April 2026
On the Structure of Local Observables in String Field Theory
Ethan J. Thompson
,Arvin Kouroshnia
Posted: 10 April 2026
Pure Analytic Calculations of the Mass Gap and Glueball Spectrum in Four-Dimensional Yang-Mills Theory
Jiazheng Liu
Posted: 09 April 2026
Minimal Finite Hankel Closure in Elastic Proton-Proton Scattering: Structural Invariants, Covariance-Aware Public-Data Benchmarks, and Preregistered LHC Tests
Mohamed Sacha
Posted: 08 April 2026
Emergence and Late-Time Evolution of SU(N) Symmetric Multiplet of Pseudoscalar Fields as an Origin of Multi-Component Dark Matter
Alexander B. Balakin
,Gleb B. Kiselev
Posted: 07 April 2026
Gauge Couplings of the Standard Model from First Principles in the Octonionic Framework
Tejinder P. Singh
Posted: 02 April 2026
Spontaneous BRST Symmetry Breaking in Infrared QCD
Angelo Raffaele Fazio
,Adam Smetana
Posted: 31 March 2026
Exceptional Parallels Between Heterotic E8 × E8 and an Octonionic E8 × E8 Program
Tejinder P. Singh
Posted: 26 March 2026
Description of the Electron in the Electromagnetic Field: The Dirac Type Equation and the Equation for the Wave Function in Spinor Coordinate Space
Pavel Gorev
Posted: 25 March 2026
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