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Coherence, Decoherence Rate, and Attractor Structure in Reduced Q5 Transport

Craig Edwin Holdway

Published Apr 20, 2026• 0 citations
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Abstract

We present three theorems that complete the structural account of coherence and decoherence in the reduced transport sector of the Q5 framework. This mathematical system derives operator structures from the combinatorial geometry of the five-dimensional hypercube and its Gray code Hamiltonian cycle. Theorem 50 identifies coherence as the survival of the commutator-driven transverse mode under transport, and establishes a precise structural distinction between reversible phase scrambling and irreversible decoherence. No new operators are introduced; all objects are inherited from the prior theorem chain (T1–T49). Theorem 51 derives the structural form of the effective decoherence rate as a product of four independently motivated factors: a base loss rate, a quadratic coupling asymmetry term, a saturating orbit depth function, and a Lorentzian detuning suppression factor. Each factor is grounded in a specific prior result in the Q5 transport chain. Theorem 52 establishes that the coherence decay rate is the unique globally attracting fixed point of a self-consistent kernel-induced dynamical map. Existence and uniqueness are proved via the intermediate value theorem applied to a strictly decreasing map; global convergence follows from even/odd subsequence monotonicity. The exponential saturation law is derived as the asymptotic reduction of the fixed-point structure in the strong-suppression regime, rather than postulated. The primary remaining open step is the explicit derivation of the coupling parameter β from the commutator [M_n, D_n]Y geometry of Theorem 29. All results are conditional on the admissible linked-pair reduction of Theorem 17 and the retained-pairing assumption of Theorem 36. Epistemic classifications are provided for each result.

DOI
10.5281/zenodo.19687098

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Q5 Decoherence as a Unique Attractor of Kernel Dynamics

Craig Edwin Holdway

This Theorem establishes that the coherence decay rate is the unique globally attracting fixed point of a self-consistent kernel-induced dynamical map. The exponential saturation law of T51 emerges as the asymptotic reduction of this fixed-point structure in the strong-suppression regime, rather than being postulated. The kernel-induced map is F(Γ_coh) := Γ_max[1 − exp(−M(Γ_coh)/M₀)], where the composite hazard variable M(Γ_coh) := P_inst(1 − exp[−β/(γ + Γ_coh)]) is self-referential, stronger decoherence suppresses revival, increasing M, increasing decoherence further. Four steps prove the unique attractor: (1) Monotonicity F'(Γ_coh) < 0 by explicit sign chain; (2) Existence and uniqueness via IVT on G = F − id with G' < −1; (3) Global convergence via even/odd subsequence monotone convergence; (4) Asymptotic reduction, in the regime β/γ ≫ 1, M(Γ_coh) ≈ P_inst and the fixed-point equation reduces to the exponential saturation law Γ_coh ≈ Γ_max(1 − e^{−P_inst/M₀}). Three corollaries: mechanism separation (β = 0 forces Γ_coh* = 0, phase instability alone is insufficient); universality across Q5 parameter families; saturation bound Γ_coh* ≤ Γ_max. The Grumpy Bear Principle provides an informal interpretation of three dynamical regimes: sleeping bear (M ≈ 0, coherent), grumpy bear (instability present but strong revival), and bear claws (M large, fixed point near Γ_max, self-referential lock-in). Status: Fixed-point monotonicity, G' < −1, existence and uniqueness, global convergence, mechanism separation, and saturation bound are all solid by explicit algebraic argument. Asymptotic reduction solid in β/γ ≫ 1 regime, regime validity not yet verified from T17 kernel. Local stability is solid in the perturbative regime. Primary open step: explicit derivation of β from [M_n,D_n]Y geometry from T17 kernel generators. All results inherit T17, T29, T33, T35, T50, T51 conditionality. Dependencies: T8, T11, T29, T33, T35, T50, T51.

•May 3, 2026•0 citations

Coherence–Alignment Structure of Reduced Q5 Transport

Craig Edwin Holdway

This collects the T26–T49 arc into a unified structural account of coherence in the reduced phase system. No new operators are introduced. Seven results are established. The observable phase is carried entirely on P⊥ = span{u₂, u₄} with generator A = iσ_y = E_d, A² = −I (T26, T37). Any reduced observable state admits Q⊥ = αI + βσ_z + γσ_x + μA with μ = ½Tr(Q⊥A) (T27); scalar, grading, and off-axis components are annihilated by the extraction functional. Coherence magnitude C := |μ| is nonzero if and only if the transported residue has a nonzero projection onto A. By T29, μ = L̃(Π_sub Π_pair Π_ret([M_n,D_n]Y)), coherence is entirely commutator-driven and transport-weighted. Decoherence occurs precisely when the commutator-driven transverse component fails to survive transport, through four mechanisms: detuning imbalance (T11), transport asymmetry (T31–T33), support leakage outside O_q(s) (T35), or boundary-induced inversion (T47–T49). From T48–T49, each boundary crossing produces a fixed rotational increment (T − I)_rot = (1/160)A plus scalar and symmetric components annihilated by the extraction functional. Three corollaries establish: density matrix correspondence |γ| ∝ |μ|; joint-state coherence condition tied to shared commutator survival; and the equivalence C ≠ 0 ≡ survival of the commutator-driven transverse mode under transport. No Lindblad equation or external decay rate is introduced. The density matrix is a representation of Q⊥, not a physical state postulate. Status: Phase-plane structure, four-parameter Hermitian representation, extraction formula, null-class annihilation, coherence identification, and commutator-driven reduction are all solid within the T26–T38 framework. Failure modes structural, each referenced theorem established the mechanism. (T − I)_rot = (1/160)A conditional on T48 near-identity model and T49 barrier symmetry action. All conditionality entirely inherited from T17, T29, T36, T38, T48, T49: no new assumptions introduced. Dependencies: T11, T26, T27, T29, T31, T32, T33, T35, T37, T38, T47, T48, T49.

•May 3, 2026•0 citations

Effective Decoherence Rate Structure

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This Theorem identifies the structural form of the effective decoherence rate arising from the irreversible coupling established in T50. The rate is not a free parameter but is determined by three structural inputs from the Q5 transport chain: Γ_eff = γ_loss · G² · [1 + β·A²] · f(d_orbit) · L(δ_detune) Four factors: (1) Base rate γ_loss·G², decay requires irreversible sector coupling; Γ_eff = 0 when γ_loss = 0, regardless of all other factors. (2) Asymmetry term [1 + β·A²], coupling asymmetry A ~ |β_J − β| = |μν'c'b − b'c| from T33; operationally A ~ |g₁ − g₀|/√(g₁² + g₀²) from T8; quadratic dependence consistent with simulation showing decay enhancement scales as (g₁ − g₀)². (3) Orbit depth term f(d_orbit) = 1 − e^{−α(d_orbit − 2)}, saturation form reflecting finite Q5 combinatorial depth; f(2) = 0 at the minimal orbit of T36–T37. (4) Lorentzian detuning suppression L(δ_detune) = 1/(1 + (δ_detune/γ_c)²), detuning suppresses coupling efficiency, not a decay channel. Three structural statements: scrambling is necessary but not sufficient for decoherence; asymmetry amplifies scrambling; irreversible coupling converts scrambling into decay. Three corollaries: zero-loss limit (Γ_eff = 0 when γ_loss = 0); resonance maximum at δ_detune = 0; symmetric coupling limit (A = 0 returns base rate). Status: Asymmetry identification A ~ |μν'c'b − b'c| from T33 solid. f(2) = 0 at minimal orbit solid within T36–T37. Three qualitative boxed statements solid from T50 and factor structure. Overall structural form model-level, functional forms of f and L are natural leading-order models, not uniquely forced. Five structural constants (γ_loss, G, α, β, γ_c) were identified qualitatively; explicit values from the T17 kernel geometry are open. All results inherit T8, T17, T33, T35, T36, T37, T50 conditionality. Dependencies: T8, T11, T29, T33, T35, T36, T37, T50.

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The Q5 Structural Spine

Craig Edwin Holdway

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•Apr 12, 2026•0 citations

Mediated Phase Emergence, Transport Reduction, and Non-Factorization

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This Theorem establishes a complete transport-to-visible reduction theorem for a five-fibre system governed by Gray-structured transport on Q5. The cyclic reflected Gray code produces a unique surviving antisymmetric ordered source, the (5,1) closure class with ordered-pair count C₅₁ = 16. This reduces under the canonical projection–pairing–retention pipeline to a nearest-neighbour antisymmetric commutator operator K on a three-dimensional carrier space. Eliminating the mediator channel via Schur reduction forces a rank-one quadratic visible operator Q⊥ ~ vvᵀ, whose phase-bearing component is extracted by μ(Q) = ½Tr(QR). Path-class decomposition gives the single-sheet coefficient law μ = 2κ_adj + κ_nonadj; cross-sheet doubling gives the observable coefficient law: μ_obs = 4κ_adj + 2κ_nonadj Independently, Schur reduction of the five-fibre Hamiltonian gives h_z = v_L·v_R/Δ, bilinear in left and right couplings. Under the transport–Hamiltonian matching hypothesis in the near-symmetric regime, μ = 2h_z + O(δ²_eff). The bilinearity is irreducible (no subsystem supported on a single visible branch can reproduce a nonzero coefficient), establishing that the observable two-state dynamics are intrinsically non-factorizable. A geometric holonomy lemma establishes that μ_obs is a loop invariant, nontrivial despite vertex-level closure, vanishing on commutative transport classes. A Berry Phase Correspondence Criterion identifies the conditions under which γ_Berry = μ_obs + O(δ²), without asserting those conditions are satisfied. Status: Gray ordered-pair counts, uniqueness of (5,1) closure source, zero-pattern of K, rank-one quadratic emergence, phase extraction, cross-sheet doubling, bilinearity, and no-one-sided-support result all solid. Conditional on phase dressing assumption (full derivation from T17 kernel generators open. Conditional on path-class multiplicity), a 2:1 ratio requires explicit enumeration from T17 kernel geometry. Conditional on transport–Hamiltonian matching, bridge requires a near-symmetric regime hypothesis and second-order leg matching justification.

•May 3, 2026•0 citations

Mediated Asymmetry and Forward Dominance in Three-Sector Quantum Systems

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This paper establishes a structural and exact result for mediated three-sector systems, demonstrating asymmetry between transport and reconstruction channels in a closed finite-dimensional setting. A minimal three-sector model is introduced in which outer states are coupled only through a mediated intermediate state. Using second-order reduction, it is shown that outer-sector transport is governed by inverse detuning structure, while asymmetry between channel-resolved amplitudes is controlled by detuning imbalance. This produces suppression of reconstruction under restricted return operations, while exact reversibility remains preserved under full unitary evolution. An exact realization of this mechanism is then provided through a three-mode packet model derived from the Q₅ framework. In this setting, forward and return amplitudes are computed explicitly, yielding a coefficient hierarchy in which forward contributions are order-one while return contributions are suppressed by approximately three orders of magnitude. This leads to a rigorously defined coherence window in which forward amplitude strictly dominates return amplitude. The results establish that forward dominance is not an isolated numerical artifact, but arises from a structural asymmetry inherent in mediated multi-channel systems. Together, the structural theorem and exact realization provide a unified account of reconstruction suppression and transport dominance in a closed-system setting. This work forms part of a broader program investigating operator structure, grading behavior, and sector-resolved dynamics on the five-dimensional hypercube (Q₅), with related results available in accompanying white papers and operator decomposition studies.

•Mar 31, 2026•0 citations
We present three theorems that complete the structural account of coherence and decoherence in the reduced transport sector of the Q5 framework. This mathematical system derives operator structures from the combinatorial geometry of the five-dimensional hypercube and its Gray code Hamiltonian cycle. Theorem 50 identifies coherence as the survival of the commutator-driven transverse mode under transport, and establishes a precise structural distinction between reversible phase scrambling and irreversible decoherence. No new operators are introduced; all objects are inherited from the prior theorem chain (T1–T49). Theorem 51 derives the structural form of the effective decoherence rate as a product of four independently motivated factors: a base loss rate, a quadratic coupling asymmetry term, a saturating orbit depth function, and a Lorentzian detuning suppression factor. Each factor is grounded in a specific prior result in the Q5 transport chain. Theorem 52 establishes that the coherence decay rate is the unique globally attracting fixed point of a self-consistent kernel-induced dynamical map. Existence and uniqueness are proved via the intermediate value theorem applied to a strictly decreasing map; global convergence follows from even/odd subsequence monotonicity. The exponential saturation law is derived as the asymptotic reduction of the fixed-point structure in the strong-suppression regime, rather than postulated. The primary remaining open step is the explicit derivation of the coupling parameter β from the commutator [M_n, D_n]Y geometry of Theorem 29. All results are conditional on the admissible linked-pair reduction of Theorem 17 and the retained-pairing assumption of Theorem 36. Epistemic classifications are provided for each result.
This Theorem establishes that the coherence decay rate is the unique globally attracting fixed point of a self-consistent kernel-induced dynamical map. The exponential saturation law of T51 emerges as the asymptotic reduction of this fixed-point structure in the strong-suppression regime, rather than being postulated. The kernel-induced map is F(Γ_coh) := Γ_max[1 − exp(−M(Γ_coh)/M₀)], where the composite hazard variable M(Γ_coh) := P_inst(1 − exp[−β/(γ + Γ_coh)]) is self-referential, stronger decoherence suppresses revival, increasing M, increasing decoherence further. Four steps prove the unique attractor: (1) Monotonicity F'(Γ_coh) < 0 by explicit sign chain; (2) Existence and uniqueness via IVT on G = F − id with G' < −1; (3) Global convergence via even/odd subsequence monotone convergence; (4) Asymptotic reduction, in the regime β/γ ≫ 1, M(Γ_coh) ≈ P_inst and the fixed-point equation reduces to the exponential saturation law Γ_coh ≈ Γ_max(1 − e^{−P_inst/M₀}). Three corollaries: mechanism separation (β = 0 forces Γ_coh* = 0, phase instability alone is insufficient); universality across Q5 parameter families; saturation bound Γ_coh* ≤ Γ_max. The Grumpy Bear Principle provides an informal interpretation of three dynamical regimes: sleeping bear (M ≈ 0, coherent), grumpy bear (instability present but strong revival), and bear claws (M large, fixed point near Γ_max, self-referential lock-in). Status: Fixed-point monotonicity, G' < −1, existence and uniqueness, global convergence, mechanism separation, and saturation bound are all solid by explicit algebraic argument. Asymptotic reduction solid in β/γ ≫ 1 regime, regime validity not yet verified from T17 kernel. Local stability is solid in the perturbative regime. Primary open step: explicit derivation of β from [M_n,D_n]Y geometry from T17 kernel generators. All results inherit T17, T29, T33, T35, T50, T51 conditionality. Dependencies: T8, T11, T29, T33, T35, T50, T51.
This collects the T26–T49 arc into a unified structural account of coherence in the reduced phase system. No new operators are introduced. Seven results are established. The observable phase is carried entirely on P⊥ = span{u₂, u₄} with generator A = iσ_y = E_d, A² = −I (T26, T37). Any reduced observable state admits Q⊥ = αI + βσ_z + γσ_x + μA with μ = ½Tr(Q⊥A) (T27); scalar, grading, and off-axis components are annihilated by the extraction functional. Coherence magnitude C := |μ| is nonzero if and only if the transported residue has a nonzero projection onto A. By T29, μ = L̃(Π_sub Π_pair Π_ret([M_n,D_n]Y)), coherence is entirely commutator-driven and transport-weighted. Decoherence occurs precisely when the commutator-driven transverse component fails to survive transport, through four mechanisms: detuning imbalance (T11), transport asymmetry (T31–T33), support leakage outside O_q(s) (T35), or boundary-induced inversion (T47–T49). From T48–T49, each boundary crossing produces a fixed rotational increment (T − I)_rot = (1/160)A plus scalar and symmetric components annihilated by the extraction functional. Three corollaries establish: density matrix correspondence |γ| ∝ |μ|; joint-state coherence condition tied to shared commutator survival; and the equivalence C ≠ 0 ≡ survival of the commutator-driven transverse mode under transport. No Lindblad equation or external decay rate is introduced. The density matrix is a representation of Q⊥, not a physical state postulate. Status: Phase-plane structure, four-parameter Hermitian representation, extraction formula, null-class annihilation, coherence identification, and commutator-driven reduction are all solid within the T26–T38 framework. Failure modes structural, each referenced theorem established the mechanism. (T − I)_rot = (1/160)A conditional on T48 near-identity model and T49 barrier symmetry action. All conditionality entirely inherited from T17, T29, T36, T38, T48, T49: no new assumptions introduced. Dependencies: T11, T26, T27, T29, T31, T32, T33, T35, T37, T38, T47, T48, T49.
This Theorem identifies the structural form of the effective decoherence rate arising from the irreversible coupling established in T50. The rate is not a free parameter but is determined by three structural inputs from the Q5 transport chain: Γ_eff = γ_loss · G² · [1 + β·A²] · f(d_orbit) · L(δ_detune) Four factors: (1) Base rate γ_loss·G², decay requires irreversible sector coupling; Γ_eff = 0 when γ_loss = 0, regardless of all other factors. (2) Asymmetry term [1 + β·A²], coupling asymmetry A ~ |β_J − β| = |μν'c'b − b'c| from T33; operationally A ~ |g₁ − g₀|/√(g₁² + g₀²) from T8; quadratic dependence consistent with simulation showing decay enhancement scales as (g₁ − g₀)². (3) Orbit depth term f(d_orbit) = 1 − e^{−α(d_orbit − 2)}, saturation form reflecting finite Q5 combinatorial depth; f(2) = 0 at the minimal orbit of T36–T37. (4) Lorentzian detuning suppression L(δ_detune) = 1/(1 + (δ_detune/γ_c)²), detuning suppresses coupling efficiency, not a decay channel. Three structural statements: scrambling is necessary but not sufficient for decoherence; asymmetry amplifies scrambling; irreversible coupling converts scrambling into decay. Three corollaries: zero-loss limit (Γ_eff = 0 when γ_loss = 0); resonance maximum at δ_detune = 0; symmetric coupling limit (A = 0 returns base rate). Status: Asymmetry identification A ~ |μν'c'b − b'c| from T33 solid. f(2) = 0 at minimal orbit solid within T36–T37. Three qualitative boxed statements solid from T50 and factor structure. Overall structural form model-level, functional forms of f and L are natural leading-order models, not uniquely forced. Five structural constants (γ_loss, G, α, β, γ_c) were identified qualitatively; explicit values from the T17 kernel geometry are open. All results inherit T8, T17, T33, T35, T36, T37, T50 conditionality. Dependencies: T8, T11, T29, T33, T35, T36, T37, T50.
This document is not a new theorem, but a structural map of the Q_5 theorem series, isolating the minimal dependency chain and the forced architecture that emerges from it. We present a structural compression showing that the combinatorial geometry of the 5-dimensional hypercube Q_5, equipped with parity grading, admissible transport, and Gray-constrained traversal, forces a uniquely determined operator algebra and state-space structure on C[Q5]. Within this forced architecture, a minimal defect-supported carrier emerges canonically, yielding a three-dimensional Lie algebra C_X isomorphic to su(2) under its natural commutator relations. Order-sensitive transport along Gray-constrained paths generates a nonfactorizable phase defect that survives projection through a sequence of reduction operators and is extracted via a canonical linear functional L. This phase is not imposed, but forced by the underlying combinatorial constraints. We further show that the embedded defect coefficient governing this phase is generically nontrivial and cannot vanish identically. This nontriviality arises from an inversion asymmetry inherent in the transport architecture. Under a compatibility condition between defect extraction and the retained transport sector, the phase reduces to a universal constant value. The resulting structure exhibits a clear correspondence with key features of quantum mechanical formalism, including graded state spaces, noncommutative operator algebras, and phase-carrying transport mechanisms. While no claim of full equivalence to quantum mechanics is made, this synthesis isolates a minimal set of combinatorial conditions under which such structures are forced, suggesting a potential geometric origin for phase coherence and its persistence under constrained transport.
This Theorem establishes a complete transport-to-visible reduction theorem for a five-fibre system governed by Gray-structured transport on Q5. The cyclic reflected Gray code produces a unique surviving antisymmetric ordered source, the (5,1) closure class with ordered-pair count C₅₁ = 16. This reduces under the canonical projection–pairing–retention pipeline to a nearest-neighbour antisymmetric commutator operator K on a three-dimensional carrier space. Eliminating the mediator channel via Schur reduction forces a rank-one quadratic visible operator Q⊥ ~ vvᵀ, whose phase-bearing component is extracted by μ(Q) = ½Tr(QR). Path-class decomposition gives the single-sheet coefficient law μ = 2κ_adj + κ_nonadj; cross-sheet doubling gives the observable coefficient law: μ_obs = 4κ_adj + 2κ_nonadj Independently, Schur reduction of the five-fibre Hamiltonian gives h_z = v_L·v_R/Δ, bilinear in left and right couplings. Under the transport–Hamiltonian matching hypothesis in the near-symmetric regime, μ = 2h_z + O(δ²_eff). The bilinearity is irreducible (no subsystem supported on a single visible branch can reproduce a nonzero coefficient), establishing that the observable two-state dynamics are intrinsically non-factorizable. A geometric holonomy lemma establishes that μ_obs is a loop invariant, nontrivial despite vertex-level closure, vanishing on commutative transport classes. A Berry Phase Correspondence Criterion identifies the conditions under which γ_Berry = μ_obs + O(δ²), without asserting those conditions are satisfied. Status: Gray ordered-pair counts, uniqueness of (5,1) closure source, zero-pattern of K, rank-one quadratic emergence, phase extraction, cross-sheet doubling, bilinearity, and no-one-sided-support result all solid. Conditional on phase dressing assumption (full derivation from T17 kernel generators open. Conditional on path-class multiplicity), a 2:1 ratio requires explicit enumeration from T17 kernel geometry. Conditional on transport–Hamiltonian matching, bridge requires a near-symmetric regime hypothesis and second-order leg matching justification.
This paper establishes a structural and exact result for mediated three-sector systems, demonstrating asymmetry between transport and reconstruction channels in a closed finite-dimensional setting. A minimal three-sector model is introduced in which outer states are coupled only through a mediated intermediate state. Using second-order reduction, it is shown that outer-sector transport is governed by inverse detuning structure, while asymmetry between channel-resolved amplitudes is controlled by detuning imbalance. This produces suppression of reconstruction under restricted return operations, while exact reversibility remains preserved under full unitary evolution. An exact realization of this mechanism is then provided through a three-mode packet model derived from the Q₅ framework. In this setting, forward and return amplitudes are computed explicitly, yielding a coefficient hierarchy in which forward contributions are order-one while return contributions are suppressed by approximately three orders of magnitude. This leads to a rigorously defined coherence window in which forward amplitude strictly dominates return amplitude. The results establish that forward dominance is not an isolated numerical artifact, but arises from a structural asymmetry inherent in mediated multi-channel systems. Together, the structural theorem and exact realization provide a unified account of reconstruction suppression and transport dominance in a closed-system setting. This work forms part of a broader program investigating operator structure, grading behavior, and sector-resolved dynamics on the five-dimensional hypercube (Q₅), with related results available in accompanying white papers and operator decomposition studies.