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Exact GEP Fusion Selector Derived, Dynamical Orientation Not Yet Selected

Štěpán Sekanina

Published Aug 7, 2026• 0 citations
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Abstract

Stone 2C addresses the next bounded question in the Granular Entropic Physics (GEP) chiral program. Stone 2A established that faithful quaternionic Q8 holonomy is compatible with an irreducible gapped Chern pump, while Stone 2B derived the corresponding four-state carrier and its complete internal matrix algebra from the local three-spinor sector of GEP. The present paper asks whether the canonical composition law of local GEP maps can distinguish this carrier, transmit its Pauli multiplicity, and select a dynamical orientation. The exact local map algebra is A6=End2T(V⊗3)≅M2(C)⊕C⊕C. Equipping A6 with the Hilbert–Schmidt geometry inherited from its action on V⊗3, let μ:A6⊗A6→A6 denote blockwise multiplication. Its positive normalization operator D=μμ† has the exact spectrum spec(D)={1×4,(21)×2}. For the central idempotent Q↔(0,1,1), complementary to the M2(C) block, −logD=(ln2)LQ=L(ln2)Q. Thus the normalization-cost generator is represented by a unique canonical positive algebra element. On the local spinor space, the corresponding element λQ has spectrum specV⊗3(λQ)={0×4,λ×4}, and its kernel is exactly the Stone-2 carrier P0V⊗3≅W⊗M,dimW=dimM=2. The normalized coisometry μˉ=D−1/2μ produces a compatibility projector Π=μˉ†μˉ. On M2(C)⊗M2(C), this projector is exactly a rank-four Bell-type identity wire, ΠM2=IL1⊗∣Φ+⟩⟨Φ+∣R1L2⊗IR2,∣Φ+⟩=2∣11⟩+∣22⟩, which transports the complete Pauli multiplicity algebra across a compatibility bond. A mandatory negative result is equally exact. Fusion is equivariant under the full adjoint U(2) action and therefore treats the two channel orientations R and R−1 identically: FAIL_ORIENTATION_SELECTION_FROM_FUSION_ALONE. The established result is an exact finite-dimensional selector-and-transport theorem. Its interpretation is that canonical GEP fusion distinguishes the Stone-2 carrier block and supplies a lossless algebraic compatibility wire. It does not yet derive a physical Hamiltonian, spatial gluing rule, collective orientation coupling, QWZ dynamics, Kaplan wall, Weyl boundary mode, or Standard-Model anomaly structure. A collective orientation interaction remains a clearly identified candidate for the next microscopic test.

DOI
10.5281/zenodo.21830840

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•Aug 25, 2026•0 citations

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Physics Letters A•Aug 13, 2026•0 citations
Stone 2C addresses the next bounded question in the Granular Entropic Physics (GEP) chiral program. Stone 2A established that faithful quaternionic Q8 holonomy is compatible with an irreducible gapped Chern pump, while Stone 2B derived the corresponding four-state carrier and its complete internal matrix algebra from the local three-spinor sector of GEP. The present paper asks whether the canonical composition law of local GEP maps can distinguish this carrier, transmit its Pauli multiplicity, and select a dynamical orientation. The exact local map algebra is A6=End2T(V⊗3)≅M2(C)⊕C⊕C. Equipping A6 with the Hilbert–Schmidt geometry inherited from its action on V⊗3, let μ:A6⊗A6→A6 denote blockwise multiplication. Its positive normalization operator D=μμ† has the exact spectrum spec(D)={1×4,(21)×2}. For the central idempotent Q↔(0,1,1), complementary to the M2(C) block, −logD=(ln2)LQ=L(ln2)Q. Thus the normalization-cost generator is represented by a unique canonical positive algebra element. On the local spinor space, the corresponding element λQ has spectrum specV⊗3(λQ)={0×4,λ×4}, and its kernel is exactly the Stone-2 carrier P0V⊗3≅W⊗M,dimW=dimM=2. The normalized coisometry μˉ=D−1/2μ produces a compatibility projector Π=μˉ†μˉ. On M2(C)⊗M2(C), this projector is exactly a rank-four Bell-type identity wire, ΠM2=IL1⊗∣Φ+⟩⟨Φ+∣R1L2⊗IR2,∣Φ+⟩=2∣11⟩+∣22⟩, which transports the complete Pauli multiplicity algebra across a compatibility bond. A mandatory negative result is equally exact. Fusion is equivariant under the full adjoint U(2) action and therefore treats the two channel orientations R and R−1 identically: FAIL_ORIENTATION_SELECTION_FROM_FUSION_ALONE. The established result is an exact finite-dimensional selector-and-transport theorem. Its interpretation is that canonical GEP fusion distinguishes the Stone-2 carrier block and supplies a lossless algebraic compatibility wire. It does not yet derive a physical Hamiltonian, spatial gluing rule, collective orientation coupling, QWZ dynamics, Kaplan wall, Weyl boundary mode, or Standard-Model anomaly structure. A collective orientation interaction remains a clearly identified candidate for the next microscopic test.
Granular Entropic Physics (GEP) is being tested through the Stone-2 program as a sequence of bounded, pre-registered questions concerning the microscopic origin of chiral quantum matter. Stone 2A established a faithful Q8-linked proxy with a gapped irreducible Chern bulk and matched chiral boundary flow. Stone 2B derived its canonical four-state carrier K = W tensor M from the local binary-tetrahedral representation, and Stone 2C derived a canonical fusion selector and a Bell-type identity wire for the two-dimensional multiplicity factor M. This paper asks whether the enriched channel-rewiring algebra already contains a distinguished orientation-odd operator and whether canonical fusion preferentially couples that direction. The active operator algebra End(M) = M2(C) decomposes under the S3 channel-relabeling action as 1 + 1_sgn + 2. The operator Omega = P0 (R - R^-1) P0 / (i sqrt(3)) transforms as Ad_g(Omega) = sgn(g) Omega and therefore spans the unique local S3 pseudoscalar line, up to normalization and the unavoidable local convention Omega -> -Omega. The most general simultaneous-S3-scalar traceless two-carrier bilinear contains two independent coefficients, V = -J_Omega C_Omega - J_E C_E, where C_Omega is the covariantly transported pseudoscalar channel and C_E is the nonchiral Pauli-doublet channel. The relevant measure of pseudoscalar preference is therefore kappa_Omega = J_Omega - J_E. For the exact Stone-2C Bell compatibility wire, the unit parent penalty is h_wire = (3/4) I - (1/4) C_E - (1/4) C_Omega. Consequently, J_Omega_wire = J_E_wire = 1/4,kappa_Omega_wire = 0. Canonical fusion thus provides nonzero covariant orientation stiffness but gives the pseudoscalar exactly the same component weight as the nonchiral doublet. It transports orientation information without selecting physical handedness. The paper also proves that the sign assigned to an isolated untransported bond is not convention free. The invariant sign data require a derived bond transport tau and closed-loop products W_Omega(C). Central Q8 holonomy -I cannot determine this anisotropy or orientation-line holonomy by itself because Q8 and Omega act on commuting tensor factors of the carrier. All results are exact finite-dimensional algebra; no code or numerical calculation is used. The established conclusion is a refinement of the missing microscopic target from a single coupling J_Omega to the tuple (kappa_Omega, tau, W_Omega), together with a physical bond operator, energy scale, and branched carrier graph. The paper does not derive a physical GEP Hamiltonian, a nonzero chiral anisotropy, an ordered many-body phase, QWZ spatial dynamics, a Kaplan-type higher-dimensional wall, a Weyl boundary mode, doubler control, or anomaly cancellation. It identifies the unique local pseudoscalar and the exact point at which canonical fusion remains insufficient.
We study the precision geometry generated by three self-adjoint observables in a faithful quantum state. The centered GNS Gramian Γ = C + iΣ, its inverse Q, normalized precision coefficients B, and conditional levels pi = ΓiiQii define a weighted magnetic triangle. The paper separates exact structure, reconstruction, and open prediction. First, a reduction identity gives pi = (1 − b 2 i )/ det(I − B). For the logarithmic embedding this implies an exact global rigidity theorem: if all three induced edge weights are positive, then the logarithmic circulant deviation obeys D > J∗ = 0.394202716596 . . . , with sharp infimum J ∗ approached only in the degenerate equal-b limit. The former numerical global-floor claim is therefore replaced by an analytic theorem, independently cross-checked by an interval branch-and-bound certificate. Second, the Pauli triple has Q = (I −i[n]×)/(1−|n| 2 ) and can realize only Hol = ±1. Real precision geometry gives instead Hol = ±i; the charged- lepton phase lies outside both quantized sectors. Third, the Koide–Foot square-root mass family is exactly the spectrum of an offset uniform magnetic Schr¨odinger operator on C3. Current 2026 PDG masses show that r = √ 2 and δ = 2/9 are each individually compatible after refitting the other parameter, but their simultaneous exactness is not: it fixes mµ/me about 451.7 quoted standard deviations from the measured ratio. Fourth, for the explicit modelling prescription µi = pi , a Krawczyk interval certificate proves an exact realization of the measured square-root mass ratios at the idealized Brannen flux Φ0 = π+2/3 on a fixed transversal slice; further Krawczyk certificates prove realizations at the exact decimal fluxes Φ = 1.105 and Φ = 1.4, and a continuation scan locates the feasibility boundary at Φ∗ ≈ 1.1044604 (record level). Finally, an implicit-function theorem turns a former caveat into a structural result: near the certified witness, the exact mass-ratio solutions form a three-dimensional manifold when (b1, Φ, α) are allowed to vary in the family µ = p α. Hence the two mass ratios cannot locally select the flux, the measure exponent, or the witness coordinate. The framework therefore provides exact rigidity, exclusions, and realizability, while identifying a parameter-free upstream selector as the precise missing ingredient required for prediction.
We study the precision geometry generated by three self-adjoint observables in a faithful quantum state. The centered GNS Gramian Γ = C + iΣ, its inverse Q, normalized precision coefficients B, and conditional levels pi = ΓiiQii define a weighted magnetic triangle. The paper separates exact structure, reconstruction, and open prediction. First, a reduction identity gives pi = (1 − b 2 i )/ det(I − B). For the logarithmic embedding this implies an exact global rigidity theorem: if all three induced edge weights are positive, then the logarithmic circulant deviation obeys D > J∗ = 0.394202716596 . . . , with sharp infimum J ∗ approached only in the degenerate equal-b limit. The former numerical global-floor claim is therefore replaced by an analytic theorem, independently cross-checked by an interval branch-and-bound certificate. Second, the Pauli triple has Q = (I −i[n]×)/(1−|n| 2 ) and can realize only Hol = ±1. Real precision geometry gives instead Hol = ±i; the charged- lepton phase lies outside both quantized sectors. Third, the Koide–Foot square-root mass family is exactly the spectrum of an offset uniform magnetic Schr¨odinger operator on C3. Current 2026 PDG masses show that r = √ 2 and δ = 2/9 are each individually compatible after refitting the other parameter, but their simultaneous exactness is not: it fixes mµ/me about 451.7 quoted standard deviations from the measured ratio. Fourth, for the explicit modelling prescription µi = pi , a Krawczyk interval certificate proves an exact realization of the measured square-root mass ratios at the idealized Brannen flux Φ0 = π+2/3 on a fixed transversal slice; further Krawczyk certificates prove realizations at the exact decimal fluxes Φ = 1.105 and Φ = 1.4, and a continuation scan locates the feasibility boundary at Φ∗ ≈ 1.1044604 (record level). Finally, an implicit-function theorem turns a former caveat into a structural result: near the certified witness, the exact mass-ratio solutions form a three-dimensional manifold when (b1, Φ, α) are allowed to vary in the family µ = p α. Hence the two mass ratios cannot locally select the flux, the measure exponent, or the witness coordinate. The framework therefore provides exact rigidity, exclusions, and realizability, while identifying a parameter-free upstream selector as the precise missing ingredient required for prediction.
Pedagogical Guide, Foundations Audit, Uniqueness & Substitutability Analysis, Literature Comparison, and Reading Guidance : A Pedagogical Guide to Understanding the OT–GKSL Architecture Short summary:This work develops the exact reduced-dynamics backbone of an Einstein-locked optimal-transport/GKSL architecture for open quantum sources and certified classical readouts. On a faithful finite-effective-support working stratum, a protocol selects a collective manifold Q, its inherited OT metric G, the drift induced by the complete GKSL generator, source potentials, admissibility constraints, and a reduced gauge connection. Once that reduced tuple and its convention are frozen, the nonlinear Euler–Lagrange equation is exact for the declared reduced action; fidelity to the parent native vector field is audited separately by the reduction residual Rred.The architecture has two parallel descendants of the native state domain. The collective/source branch descends toward Q. The record/geometric branch first fixes event identity from protocol-complete certified records, then performs the declared geometric coarse-graining and rank-D coordinate readout. Hencecomplete event-record content ̸= rank-D coordinate content in general. On the observed branch D = 4 is a branch lock, while the positive state-space metric gOT and the Lorentzian readout metric gro remain distinct objects. The paper separates three response types that must not be conflated. The scalar constitutive channel is controlled by βμ(pκ) = −∂pκ ln μ(pκ), F(μ) = −ζμβμ grad_G(pκ).The reduced gauge-holonomic channel is carried by Ared and Fred and is exposed by oriented protocol loops. Separately, the geometric OT-to-readout bridge uses the projected horizontal connection ∇H, its curvature RH, and its holonomy HolH. A nonzero reduced gauge loop response is therefore not, by notation alone, the same object as horizontal/readout holonomy. A chiral HS/NJL realization supplies the nonlinear two-coordinate sector Y (ρ) = σ(ρ)(Id) + iγ^5π(ρ) = r(ρ)exp (iγ^5φ(ρ)), with the phase-drift-free Routh potential Ueff(r; J) = Usrc(r) + [J − νAφ(r)]^2/(2 g_φ(r)).Stationary formulas based only on U′eff(r∗) = 0 are used on the declared conservative-core radial lock Lr(r∗) = 0, or as a controlled approximation when radial drift lies inside its remainder. Stronger global mass/vacuum branch statements remain conditional on the dedicated branch hypotheses and matching dictionary.The same architecture supports controlled Abelian/Maxwell, Dirac/Pauli/Schrödinger and Newtonian descendants on their respective certified windows. Einstein compatibility has a different status: it is a nonlinear closure gate comparing independently constructed geometry, source and interface sectors while the Einstein–Hilbert kinetic normalization remains fixed with constant G0. Narrowband laboratory estimators use calibrated readout time tro, distinct from the native evolution parameter ξ. The exact reduced equation and its claim status The central reduced equation is ∇(G)_q˙ (q˙ − L) + (∇(G)L)†(q˙ − L) = −grad_G . Usrc + Somme[ λα gradGCα + ν ♯G(ιq˙Fred)] 1. Foundations of the Architecture: Foundations |GKSL/Lindblad ; Carlen–Maas ; Jacobson ; Sakharov ; Donoghue ; Lovelock) Establishes the core Einstein-locked OT/GKSL architecture for certified geometric readout and coherence-dependent gravitational sourcing. Optimal-Transport Gravity Trilemma | Identifies the certified operational boundary of geometric readout by proving the fundamental trade-off between temporal resolution, coframe stability, and bridge fidelity. 2. Emergence and Recovery of Classical Physics: Exact Reduced OT/GKSL Equations | Mori–Zwanzig/projection operators ; effective field theory ; Carlen–Maas ; Wilsonian reduction / Demonstrates the controlled recovery of classical Newtonian and gravitational sectors as exact non-linear reductions of the native OT/GKSL state dynamics. Certified Einstein Non-Linear Readout | Lovelock ; Bianchi identities ; Donoghue EFT ; Jacobson thermodynamic gravity// Develops the full non-linear Einstein-locked readout closure for the metric sector. Non-Linear Dynamics and Readout | Dynamical systems, center manifold/effective reduction ; quantum Markov semigroups ; non-linear open-system reductions // Explores the exact reduced non-linear evolution on collective state manifolds. The Seeley–DeWitt Bridge | Seeley–DeWitt heat-kernel ; Vassilevich // Formalizes the operational connection between native state dynamics and the effective classical readout. The SDW Bridge: Composite Brout–Englert–Higgs Dynamics, Spectral Separation, and the Emergent Graviton | Formalizes the emergence of the Brout-Englert-Higgs composite scalar and the spin-2 graviton via the Seeley-DeWitt expansion, strictly preserving the Einstein-Lock. Bridge between QCD and OT/GKSL Readout | Wilson lattice gauge theory ; Gross–Wilczek–Politzer asymptotic freedom ; Kogut–Susskind Hamiltonian lattice gauge theory // Connects the Optimal Transport / GKSL framework to Quantum Chromodynamics, exploring the constitutive bridge and effective low-energy dynamics. 3. The Certified Boundary and Structural Limits: Certified Spacetime Readout on Finite Support: A Unified Temporal and Geometric Boundary | Decoherence / Quantum Darwinism ; quantum reference frames ; finite information bounds ; Jacobson // Unifies the temporal and geometric branches of classical readout into a single certified spacetime problem. Introduces the unified spacetime readout burden and derives the central unified certified-budget inequality, proving that temporal precision, geometric coframe nondegeneracy, and bridge compatibility draw from the same finite entropic and informational resources and cannot be made simultaneously ideal. Certified Causality, Locality, Nonlocality, and Relativity in the Einstein-Locked OT/GKSL Framework | Algebraic QFT/locality ; operational quantum theory ; quantum reference frames ; relativistic causality tests // Determines the exact status of causality, locality, nonlocality, and the principle of relativity within the Einstein-locked OT/GKSL architecture. Shows that causal-local spacetime semantics is a certified readout property rather than a primitive native axiom; proves a patchwise gluing theorem for certified local causal structure; and derives a unified finite-budget inequality showing that temporal precision, geometric certification, bridge admissibility, and overlap compatibility all compete for a single residual causal-local headroom on finite effective support. Entropic Tick Cost and Certified Temporal Readout in the Einstein-Locked OT/GKSL Framework | Demonstrates that classical ticks are finite-resource readout objects extracted from native entropic ordering, rather than primitive background parameters. Decomposes the entropic tick cost into native, extraction, and certification branches, and derives a theorem-level certified temporal budget inequality connecting temporal resolution, finite effective support, and certification margins. Entropic Tick Cost & Spectral Budget | Page–Wootters time ; thermal time hypothesis ; quantum clocks ; Salecker–Wigner bounds // Establishes a theorem-strength certified boundary for classical spacetime by proving a fundamental trade-off between entropic tick resolution, coframe stability, and finite informational budget. Toy Certified Pipeline from Optimal Transport QCD | Provides a protocol-level implementation and scaling model for certified bridge margins. Certified Spectral Boundary from Heat-Kernel Budgets and Entropic Transport in the Einstein-Locked OT/GKSL Framework | Heat-kernel spectral budgets; entropic OT/GKSL transport; certified spectral boundary; Einstein-locked readout. Develops a spectral-geometric control layer for the OT/GKSL framework, where the native heat trace bounds finite spectral resources, the cutoff gap defines a certification margin, and entropic transport controls the drift of readout-support budgets without inducing a state-dependent Einstein–Hilbert kinetic term. Correlation Separation in the Einstein-Locked OT/GKSL Framework | Establishes a theorem-level distinction between native, readout, and causal-local correlations, and reframes the horizon information problem through certified-domain correlation layering 4. Cosmological Dynamics & Global Readout Constraints: Vacuum-like Residual Energy from Constitutive-Holonomic Balance in a Minimal Reduced OT-C3 Sector | Effective potentials ; Coleman-Weinberg ; Sakharov induced gravity ; vacuum energy problem // Demonstrates analytically that the macroscopic cosmological constant emerges as a non-zero vacuum-like residual energy resulting from the exact balance between scalar constitutive dissipation (source sector) and the non-commutative holonomic barrier of the Optimal Transport geometry. Homogeneous Closed Readout Dynamics under Finite Spacetime Budget | FLRW cosmology ; effective dark energy ; backreaction ; EFT of dark energy// Constructs a homogeneous and isotropic model (G-FLRW) demonstrating how the spacetime budget acts as a branch-selection mechanism, effectively identifying the vacuum-like sector (Λ) as the maintenance cost of certified spacetime solvability. 5. Experimental Protocols and Testability: Testing Source-Side State Dependence in Gravity with Lock-In Atom Interferometry | Kasevich–Chu ; Peters–Chung–Chu ; Rosi–Tino ; atom gravimetry // Proposes a concrete experimental protocol to falsify source-only emergent gravity at low energy. A Lock-in Atom-Interferometric Test (Clock) | Detailed operational implementation of the low-energy readout test for the Einstein-locked framework. Experimental Separation of Readout and Causal-Local Correlation Layers in the Einstein-Locked OT/GKSL Framework //Circuit QED / transmons ; readout fidelity ; mutual information ; quantum verification // Proposes a falsifiable experimental protocol (CL
Paper 3 of a four-paper program on generalized quantum measurement, realization geometry, and informational invariance. Generalized quantum measurements admit multiple purification and dilation realizations of the same operational state–measurement data. This paper studies the geometric structure induced by that representation freedom and develops a transport theory on the resulting realization space. On each finite-dimensional regular fixed-rank state–POVM stratum, framed purification amplitudes and framed Naimark realizations are shown to assemble into a smooth principal bundle whose fibers are precisely compact auxiliary gauge orbits. The paper establishes complete-POVM robustness results controlling states, labeled measurement architectures, fixed coarse events, canonical normalization, and smooth operational paths. A framed Hilbert–Schmidt response geometry is then introduced on the realization bundle. The associated minimum-response construction yields a smooth gauge-equivariant principal connection and an induced positive response metric on the operational base manifold. This provides a geometrically distinguished transport law and establishes relative canonicity within the framed response geometry. The manuscript further introduces Quantum Informational Identity (QII) and Dynamical Quantum Informational Identity (DQII) as explicit foundational identity assumptions. Exact gauge transformations are shown to preserve the generated informational profile of a realization, while smooth gauge paths preserve the corresponding dynamical profile history. Under QII and DQII, all quantum-informationally admissible principal connections determine the same represented quantum-physical transport content. Relative to the framed Hilbert–Schmidt response geometry, the minimum-response connection is the unique minimum-response representative of that common content. The paper refers to this combination of: uniqueness of represented quantum-physical transport content, and uniqueness of the framed minimum-response representative, as absolute canonicity within the generated realization framework. The results are restricted to finite-dimensional generated realizations on regular fixed-rank strata with fixed outcome labels. The paper does not claim that the framed response geometry is uniquely derived from informational principles, nor does it extend the transport theory across singular or rank-changing loci.
Complex Hilbert space is usually assumed at the start of quantum mechanics. This paper formulates a reverse construction for the one-particle and operator-algebraic setting. Starting from a real Hilbert space carrying an orthogonal representation, the admissible imaginary units are identified with the skew-adjoint square roots of − Id in the Real commutant of the complexified representation. The novelty is not the isolated use of complexification, spectral orientation, or polar decomposition, but their order of dependence: first the symmetry representation defines an intrinsic operator-valued phase space; then an oriented internal time flow selects a distinguished point of that phase space; only afterward are the usual complex one-particle, observable, probability, and Weyl–CCR structures invoked under their standard hypotheses. In the terminology used here, this oriented internal flow is the reversible or inner-generative side of a dual-time distinction. It is not a second observer clock and not an additional Lorentzian coordinate: mathematically it is the strongly continuous orthogonal group U ( t ) = exp ( t A ) on the real Hilbert space. Its Stone-dual variable is energy/frequency λ ; canonical conjugation pairs λ with − λ ; positive energy orients this pair and selects the canonical phase on the dynamic sector through A = J | A | = | A | J . Thus inner-generative time is the source of phase orientation, while irreversible record time, projection, memory, and decoherence enter only as later reduced-dynamics layers. No spectral gap at zero is required, and zero modes remain visible as residual phase data rather than being hidden by the construction. The selected phase is invariant under time-orientation-preserving symmetries and changes sign under time reversal, giving the usual antiunitary action after complex reconstruction. The paper also makes explicit the monoidal limitation: two selected local phases do not make the raw real tensor product the standard composite system; the standard composite is recovered only after imposing the J -balanced, equivalently complex, tensor product rule. Thus the result is a reconstruction of compatible complex kinematics on the selected one-particle/operator-algebraic sector, not a derivation of all quantum foundations from purely real data.