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Geometric Resolution of the "Vacuum Catastrophe" Within the Framework of the 10D Electromagnetic Structure of the Atomic Nucleus
Anastasia Vikhareva
Posted: 20 October 2026
Block Heat-Bath Proposals for Topology Sampling in the Schwinger Model
Danyang Li
Posted: 19 October 2026
A Conditional Reconstruction Model of the Dark Sector: Symmetry, Topological Defects, and Invariant Capacities
Bin Li
Posted: 19 October 2026
Some Properties of Dimensional Regularization and Their Application
S.A. Larin
Posted: 19 October 2026
Charged-Fermion Mass Phenomenology and the Pati-Salam Mass Plane: Route Normalization, Physical Matching, and Current Probes in Sp(18)
Yaroslav D. Krivenko-Emetov
Posted: 16 October 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: 12 October 2026
Topological Origin of the Higgs Field: Emergence of Electroweak Sector from String-Net Condensation
Xiaodong Yang
,Yuchen Yang
,Helin Mei
Posted: 10 October 2026
Decoherence Cartography with Transportable Matter and Antimatter Qubits as Probes of Beyond the Standard Model Sectors
Alexander S. Sakharov
,Rostislav Konoplich
Posted: 07 October 2026
A Conditional Structural Reconstruction of Newton’s Constant: Dimensionless Quantum–Gravitational Coupling from Defect–Platform Co-Selection
Bin Li
Posted: 06 October 2026
A Unified Electro-Gravity (UEG) Theory for Modeling a General Class of Elementary Particles
Nirod Das
Posted: 30 September 2026
Joint Direction and Distance Estimation of Low-Energy Photon Point Sources Using a Spatial–Global Dual-Branch CNN
Yier Liu
,Jiangang Zhang
,Yapeng Yang
,Qingbo Du
,Xiaoyu Zhao
,Qi Lv
Posted: 29 September 2026
Renormalized Route Reciprocity and Charged-Fermion Mass Shape in a Chiral SU(15)p Composite Theory
Yaroslav D. Krivenko-Emetov
Posted: 24 September 2026
Flux-Textured Yukawa Couplings and Fermion Mass Hierarchies
Ahmed Ali
Posted: 21 September 2026
Beyond Field-Line Descriptions: Unintended Antennas, EMC, and Signal Integrity
Fred Lane Martin
Posted: 09 September 2026
Gauge-Coupling Corrections from Dual-Axis Return: Linking 0.07115 and 0.1180
Xianwei Meng
Posted: 09 September 2026
Beyond Field-Line Descriptions: Electromagnetic Energy Transport in Intended Antennas
Fred Lane Martin
Posted: 09 September 2026
Beyond Field-Line Descriptions: Alternating Electromagnetic Energy Transport in AC Systems
Fred Lane Martin
Posted: 08 September 2026
Route Reciprocity and the Logarithmic Yukawa-Curvature Plane of Charged Fermions in the SU(15)p Composite Theory: Four-Dimensional Composite Dynamics, Five-Dimensional Spectral Reconstruction, and a Prospective Six-Dimensional Completion
Yaroslav D. Krivenko-Emetov
This article asks whether an anomaly-consistent confining preon theory with gauge group \(\mathrm{SU}(15)_p\) can account for a simple relation among the nine charged-fermion Yukawa eigenvalues. For each charged sector \(s\in\{\ell,d,u\}\), define \(A_s=\frac14\left(\ln y_{s,1}-2\ln y_{s,2}+\ln y_{s,3}\right), \qquad \Delta_\Pi=A_\ell+2A_d-A_u\), with all Yukawa eigenvalues evaluated at one common scale in one renormalization scheme. Current running inputs give \(\Delta_\Pi(M_Z)=0.0189642\). The most complete public covariance reconstruction available for the combined inputs gives \(\sigma_{\Delta_\Pi}\simeq0.01219\), or \(Z_\Pi\simeq1.56\). The near-plane relation is therefore treated as a falsifiable structural clue, not as an established empirical law. The central four-dimensional result is exact. In the fixed four-route Pati–Salam operator basis, \(\Delta_\Pi=C_{21}-C_{12}\), so \(\Delta_\Pi=0\) is equivalent to equality of the two crossed route coefficients. The unchanged chiral field content admits an explicit gauge-invariant point-split source with 24 fermionic insertions. A Schouten-reduced six-current quotient contains noncommuting Temperley–Lieb route operations, while a walled–Brauer construction generates the required \(\mathrm{SU}(4)_{\rm PS}\) crossed color kernels, including the effective direct/crossed coefficient \(-1/2\). A stronger closure-preserving chronological interpretation is excluded under the stated assumptions. Any equality of the complete crossed amplitudes must therefore be dynamical rather than a microscopic route Ward identity. Family alignment is an independent requirement. For the corrected symmetric flavour spurion \(H_S=\lambda'\lambda'^\dagger\), the median projector \(P_2(H_S)\) defines the basis-covariant tensor \(D_+=I_3-3P_2(H_S)\) with eigenvalues (1,-2,1). A gauge-neutral light-family composite \(\Sigma\in\overline{\mathbf6}_F\) of residual \(SU(3)_F\) supplies a constructive nonlinear alignment channel. A separate four-flavour parent embedding introduces a restricted \(U(1)_X\times SU(4)_F\) spurion branch. Within that branch, the parent cubic invariant that would induce the light-family determinant operator is forbidden to all polynomial orders. This is a conditional completion result, not a symmetry theorem of the minimal three-\(\psi\) Pati–Salam field content. More general light-family EFT branches admit a finite determinant-tolerant global domain. The physical confining theory must still determine which branch is realized and the corresponding renormalized scalar coefficients. The decisive route-dynamics observable is the renormalized two-source correlator. After canonicalization of the positive source metric, let \(K(E)\) be the Hermitian two-route kernel and \(K_\perp=[K-\sigma_xK\sigma_x]/2\). If an isolated route-odd state exists with gap \(\Delta_-^{(15)}\), define \(\eta_{15}=\frac{\|K_\perp(E_*)\|_2}{\Delta_-^{(15)}}\). Static operator algebra fixes neither the numerator nor the denominator. Pole tracking, Schur–Feshbach reduction, finite Euclidean moment/Krylov criteria, and pole-amputated three-point functions provide a source-normalization-robust decision protocol. In any finite invertible parity-preserving scheme, the pole statements \(F_+(0)\ne0\) and \(F_-(0)=0\) are invariant. An exact pole-resolved plane additionally requires the regular route-odd remainder \(C_-^{\rm reg}\) to vanish in the same scheme. The microscopic-to-phenomenological bridge can be written as a finite channel Jacobian. For the explicit route-21 source, \(B_{21}=-2E_{03}+6E_{153}\) fixes the local source Clebsches. Propagation reduces the remaining channel dependence to the response ratio \(r_{153/03}=\mathcal P_{153}(0)/\mathcal P_{03}(0)\) and one overall amplitude. This route-21 reduction is a one-sided matching result; it does not replace the full two-route correlator test. Before the full four-dimensional calculation, the proposed dynamics has been tested in a hierarchy of simpler non-Abelian confining and spectral control problems. In a genuine \(1+1\) dimensional \(\mathrm{SU}(3)\) baryon-transfer Hamiltonian, the first nonzero crossed amplitudes are exactly reciprocal when the route-sensitive intermediate costs are equal, while unequal costs are suppressed by the confinement flux gap; the exact two-site control also has equal diagonal route correlators for all Euclidean times in the exchange-symmetric case. In the representation-matched \(1+1\) dimensional \(\mathrm{SU}(N)\) open chain, the route-odd gap scales as \(\Delta_{-,L}^{(N)}=\kappa_E N/2+O(1)\) uniformly in the chain length. For \(N=15\), pole-tracked calculations through 30 links give large-volume linear susceptibilities \(\mathcal T_{\delta t}^{\rm lin,ctrl}\simeq0.01279\) and \(\mathcal T_y^{\rm lin,ctrl}\simeq0.045586\), while the mode-resolved cancellation factor approaches about \(1.46\times10^{-2}\). Point-split, plaquette, cross-junction, screening/string-breaking, transverse \(2+1/3+1\) dimensional, and variational source controls identify important failure modes and show that source oddness, a light odd pole, and a small route-breaking numerator are distinct questions. These results establish dynamical plausibility and stopping rules, not a four-dimensional prediction for \(\eta_{15}\). The five-dimensional branch contains stronger exact results than a geometric analogy. If the physical route-\(\mathbb Z_2\) quotient is accepted as one low-energy datum, rank-one projection followed by exact Schur–Feshbach reduction closes the route-odd sector. Under the stated cyclicity and moment assumptions, the positive projected spectral measure then admits an exact local Stieltjes–Jacobi representation whose endpoint resolvent reproduces the original correlator. In the one-band Jacobi–Robin class, the band edges and first moment determine the asymptotic bulk coefficients and the canonically normalized endpoint defect, while higher moments test locality rather than assume it. Route-resolved matrix data additionally give finite-time inertia/GEVP and Cantelli-type certificates for subthreshold support and visible odd fidelity, without requiring an uncontrolled \(t\to\infty\) fit; a commutator identity quantifies stability of a common reflection axis. The stronger claim that this quotient itself emerges from unchanged four-dimensional \(\mathrm{SU}(15)_p\) dynamics remains open. Six dimensions are a prospective ultraviolet completion with several established localization and stability results but one unresolved physical dipole Birman–Schwinger gate. The tested seven-dimensional branch remains a negative control because the tested spinor projection yields twice the intended four-dimensional zero-mode multiplicity. The main unresolved calculation is explicit rather than hidden in an effective parameter: the renormalized four-dimensional \(2 \times 2\) route correlator and associated three-point matching vertex must determine \(\Delta_-^{(15)}\), \(K_\perp\), \(\eta_{15}\), and the physical form factors.
This article asks whether an anomaly-consistent confining preon theory with gauge group \(\mathrm{SU}(15)_p\) can account for a simple relation among the nine charged-fermion Yukawa eigenvalues. For each charged sector \(s\in\{\ell,d,u\}\), define \(A_s=\frac14\left(\ln y_{s,1}-2\ln y_{s,2}+\ln y_{s,3}\right), \qquad \Delta_\Pi=A_\ell+2A_d-A_u\), with all Yukawa eigenvalues evaluated at one common scale in one renormalization scheme. Current running inputs give \(\Delta_\Pi(M_Z)=0.0189642\). The most complete public covariance reconstruction available for the combined inputs gives \(\sigma_{\Delta_\Pi}\simeq0.01219\), or \(Z_\Pi\simeq1.56\). The near-plane relation is therefore treated as a falsifiable structural clue, not as an established empirical law. The central four-dimensional result is exact. In the fixed four-route Pati–Salam operator basis, \(\Delta_\Pi=C_{21}-C_{12}\), so \(\Delta_\Pi=0\) is equivalent to equality of the two crossed route coefficients. The unchanged chiral field content admits an explicit gauge-invariant point-split source with 24 fermionic insertions. A Schouten-reduced six-current quotient contains noncommuting Temperley–Lieb route operations, while a walled–Brauer construction generates the required \(\mathrm{SU}(4)_{\rm PS}\) crossed color kernels, including the effective direct/crossed coefficient \(-1/2\). A stronger closure-preserving chronological interpretation is excluded under the stated assumptions. Any equality of the complete crossed amplitudes must therefore be dynamical rather than a microscopic route Ward identity. Family alignment is an independent requirement. For the corrected symmetric flavour spurion \(H_S=\lambda'\lambda'^\dagger\), the median projector \(P_2(H_S)\) defines the basis-covariant tensor \(D_+=I_3-3P_2(H_S)\) with eigenvalues (1,-2,1). A gauge-neutral light-family composite \(\Sigma\in\overline{\mathbf6}_F\) of residual \(SU(3)_F\) supplies a constructive nonlinear alignment channel. A separate four-flavour parent embedding introduces a restricted \(U(1)_X\times SU(4)_F\) spurion branch. Within that branch, the parent cubic invariant that would induce the light-family determinant operator is forbidden to all polynomial orders. This is a conditional completion result, not a symmetry theorem of the minimal three-\(\psi\) Pati–Salam field content. More general light-family EFT branches admit a finite determinant-tolerant global domain. The physical confining theory must still determine which branch is realized and the corresponding renormalized scalar coefficients. The decisive route-dynamics observable is the renormalized two-source correlator. After canonicalization of the positive source metric, let \(K(E)\) be the Hermitian two-route kernel and \(K_\perp=[K-\sigma_xK\sigma_x]/2\). If an isolated route-odd state exists with gap \(\Delta_-^{(15)}\), define \(\eta_{15}=\frac{\|K_\perp(E_*)\|_2}{\Delta_-^{(15)}}\). Static operator algebra fixes neither the numerator nor the denominator. Pole tracking, Schur–Feshbach reduction, finite Euclidean moment/Krylov criteria, and pole-amputated three-point functions provide a source-normalization-robust decision protocol. In any finite invertible parity-preserving scheme, the pole statements \(F_+(0)\ne0\) and \(F_-(0)=0\) are invariant. An exact pole-resolved plane additionally requires the regular route-odd remainder \(C_-^{\rm reg}\) to vanish in the same scheme. The microscopic-to-phenomenological bridge can be written as a finite channel Jacobian. For the explicit route-21 source, \(B_{21}=-2E_{03}+6E_{153}\) fixes the local source Clebsches. Propagation reduces the remaining channel dependence to the response ratio \(r_{153/03}=\mathcal P_{153}(0)/\mathcal P_{03}(0)\) and one overall amplitude. This route-21 reduction is a one-sided matching result; it does not replace the full two-route correlator test. Before the full four-dimensional calculation, the proposed dynamics has been tested in a hierarchy of simpler non-Abelian confining and spectral control problems. In a genuine \(1+1\) dimensional \(\mathrm{SU}(3)\) baryon-transfer Hamiltonian, the first nonzero crossed amplitudes are exactly reciprocal when the route-sensitive intermediate costs are equal, while unequal costs are suppressed by the confinement flux gap; the exact two-site control also has equal diagonal route correlators for all Euclidean times in the exchange-symmetric case. In the representation-matched \(1+1\) dimensional \(\mathrm{SU}(N)\) open chain, the route-odd gap scales as \(\Delta_{-,L}^{(N)}=\kappa_E N/2+O(1)\) uniformly in the chain length. For \(N=15\), pole-tracked calculations through 30 links give large-volume linear susceptibilities \(\mathcal T_{\delta t}^{\rm lin,ctrl}\simeq0.01279\) and \(\mathcal T_y^{\rm lin,ctrl}\simeq0.045586\), while the mode-resolved cancellation factor approaches about \(1.46\times10^{-2}\). Point-split, plaquette, cross-junction, screening/string-breaking, transverse \(2+1/3+1\) dimensional, and variational source controls identify important failure modes and show that source oddness, a light odd pole, and a small route-breaking numerator are distinct questions. These results establish dynamical plausibility and stopping rules, not a four-dimensional prediction for \(\eta_{15}\). The five-dimensional branch contains stronger exact results than a geometric analogy. If the physical route-\(\mathbb Z_2\) quotient is accepted as one low-energy datum, rank-one projection followed by exact Schur–Feshbach reduction closes the route-odd sector. Under the stated cyclicity and moment assumptions, the positive projected spectral measure then admits an exact local Stieltjes–Jacobi representation whose endpoint resolvent reproduces the original correlator. In the one-band Jacobi–Robin class, the band edges and first moment determine the asymptotic bulk coefficients and the canonically normalized endpoint defect, while higher moments test locality rather than assume it. Route-resolved matrix data additionally give finite-time inertia/GEVP and Cantelli-type certificates for subthreshold support and visible odd fidelity, without requiring an uncontrolled \(t\to\infty\) fit; a commutator identity quantifies stability of a common reflection axis. The stronger claim that this quotient itself emerges from unchanged four-dimensional \(\mathrm{SU}(15)_p\) dynamics remains open. Six dimensions are a prospective ultraviolet completion with several established localization and stability results but one unresolved physical dipole Birman–Schwinger gate. The tested seven-dimensional branch remains a negative control because the tested spinor projection yields twice the intended four-dimensional zero-mode multiplicity. The main unresolved calculation is explicit rather than hidden in an effective parameter: the renormalized four-dimensional \(2 \times 2\) route correlator and associated three-point matching vertex must determine \(\Delta_-^{(15)}\), \(K_\perp\), \(\eta_{15}\), and the physical form factors.
Posted: 08 September 2026
Beyond Field-Line Descriptions: Electric Energy Release Regimes
Fred Lane Martin
Posted: 07 September 2026
Beyond Field-Line Descriptions: A Unified Threshold Framework for Electric and Magnetic Energy-Release Regimes
Fred Lane Martin
Posted: 07 September 2026
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