Encyclopedia Holography Holography Seam Ledger Discharge B2 Unique Zero Of Anomaly Ledger
ARTICLE 4 claims 4 theorems
Holography Seam Ledger Discharge B2 Unique Zero Of Anomaly Ledger
A machine-checked theorem pins down the one period at which a seam's cost vanishes, and shows the result survives even when the exact cost formula is weakened.
The unique deficit-free period
In the Recognition Science framework, a ledger is a discrete record of events, and its cost is the forced price of recognizing those events. The theorem b2_unique_zero_of_anomalyLedger establishes a precise fact about one such cost function: for any positive rate parameter κ and any positive period T, the cost C(κ, T) equals zero if and only if T equals 2π/κ. This period, called the deficit-free period, is the unique time interval at which the ledger's per-cycle seam cost vanishes. The result holds for the specific cost reading f(t) = t/2 − 1, which is the anomaly reading in the framework's terminology.
The proof rests on a trace bound for 2×2 matrices that preserve a certain pairing form. For such a matrix W with a positive real eigenvalue x, its trace equals x + x⁻¹, which is always at least 2, with equality exactly when x = 1. This bound, combined with the calibration condition f(2) = 0 and the faithfulness condition f(t) ≠ 0 for t > 2, forces the zero set. The key insight is that the exact form of the anomaly reading is not load-bearing: the same conclusion follows for any reading function satisfying those two conditions. The theorem is proved in the machine-checked library of formal theorems, with no unproved assumptions.
The framework also proves that the anomaly reading is equivalent to a more general conservation condition, and that the cost function equals the framework's canonical cost J(x) = (x + 1/x)/2 − 1. However, the theorem does not claim that the physical seam cost actually satisfies the ledger closure pricing condition. That physical instantiation, whether a real system's cost report and audit discipline realize the framework's axioms, remains an open target. The theorem's power is conditional: if the ledger closure condition holds, then the unique zero is forced.
What the theorem does not claim is equally important. It does not identify the rate parameter κ with any physical horizon clock rate; that identification is a separate open question. It does not assert that the anomaly reading is the only possible reading, only that the zero set is independent of the reading's exact form. And it does not prove that the cost function J is the unique cost satisfying the closure condition; that uniqueness is a separate theorem in the framework. The declaration is a precise, conditional statement about a mathematical structure, not a claim about any specific physical system.
THEOREM b2_unique_zero_of_anomalyLedger · IndisputableMonolith/Holography/SeamLedgerDischarge.lean
/-- **B2 through the landed chain (THEOREM, CITED).** At the anomaly reading the B2
discharge also follows from `b2_unique_zero_of_conserving` — consistency check that
the weak route and the landed route agree on the zero set. -/
theorem b2_unique_zero_of_anomalyLedger (C : ℝ → ℝ → ℝ)
(h : LedgerClosurePricing anomalyReading C)
(kappa T : ℝ) (hk : 0 < kappa) (hT : 0 < T) :
C kappa T = 0 ↔ T = DeficitFreePeriod.euclideanPeriod kappa :=
b2_unique_zero_of_conserving C
(conservingSeamPricing_of_anomalyLedger C h) kappa T hk hT
THEOREM conserving_trace_bound · IndisputableMonolith/Holography/SeamLedgerDischarge.lean
/-- **The key new lemma, bundled (THEOREM):** for pairing-conserving `W` with real
eigenvalue `x > 0`, `Tr W = x + x⁻¹ ≥ 2`, with equality iff `x = 1`. This is what
lets the discharge below run on ANY calibrated faithful trace reading, not just the
character anomaly: the trace separates "deficit-free" from "mismatched" all by
itself. -/
theorem conserving_trace_bound {W : Matrix (Fin 2) (Fin 2) ℝ} {x : ℝ}
(hcons : ∀ u v, pairForm (W.mulVec u) (W.mulVec v) = pairForm u v)
(hx : 0 < x) (h : HasRealEigen W x) :
W.trace = x + x⁻¹ ∧ 2 ≤ W.trace ∧ (W.trace = 2 ↔ x = 1) :=
⟨conserving_trace_eq hcons hx h, conserving_trace_ge_two hcons hx h,
conserving_trace_eq_two_iff hcons hx h⟩
THEOREM b2_unique_zero_of_ledgerClosure · IndisputableMonolith/Holography/SeamLedgerDischarge.lean
/-- **B2 from the weak residue (THEOREM, FORCED-CONDITIONAL on
`LedgerClosurePricing`).** For ANY calibrated faithful trace reading, the
deficit-free period `β = 2π/κ` is the UNIQUE zero of the per-cycle cost:
* off the period, `turnRatio ≠ 1` (`turnRatio_eq_one_iff`, CITED), so the trace is
strictly above 2 (`conserving_trace_bound`) and faithfulness forbids a zero;
* at the period, `turnRatio = 1`, the trace is exactly 2, and calibration fires.
The character anomaly appears NOWHERE: the B2 zero set is forced by conservation,
delivery, calibration, and faithfulness alone. -/
theorem b2_unique_zero_of_ledgerClosure (R : TraceReading) (C : ℝ → ℝ → ℝ)
(h : LedgerClosurePricing R C) (kappa T : ℝ) (hk : 0 < kappa) (hT : 0 < T) :
C kappa T = 0 ↔ T = DeficitFreePeriod.euclideanPeriod kappa := by
obtain ⟨W, hcons, heig, hC⟩ := h kappa T hk hT
have hx : 0 < turnRatio kappa T := turnRatio_pos hk hT
rw [hC]
constructor
· intro h0
by_contra hne
have hx1 : turnRatio kappa T ≠ 1 := fun h1 =>
hne ((turnRatio_eq_one_iff kappa T hk).mp h1)
have htr2 : W.trace ≠ 2 := fun heq =>
hx1 ((conserving_trace_eq_two_iff hcons hx heig).mp heq)
have hgt : 2 < W.trace :=
lt_of_le_of_ne (conserving_trace_ge_two hcons hx heig) (Ne.symm htr2)
exact R.faithful W.trace hgt h0
· intro hTeq
have hx1 : turnRatio kappa T = 1 := (turnRatio_eq_one_iff kappa T hk).mpr hTeq
have htr : W.trace = 2 := by
rw [conserving_trace_eq hcons hx heig, hx1]
norm_num
rw [htr]
exact R.calibrated
THEOREM cost_eq_J_of_anomalyLedger · IndisputableMonolith/Holography/SeamLedgerDischarge.lean
/-- **The cost is J of the turn ratio (THEOREM, FORCED-CONDITIONAL).** At the
anomaly reading, the weak premise forces `C κ T = J(κT/2π)` — the full T5 pricing,
recovered by citation of the landed chain. -/
theorem cost_eq_J_of_anomalyLedger (C : ℝ → ℝ → ℝ)
(h : LedgerClosurePricing anomalyReading C)
(kappa T : ℝ) (hk : 0 < kappa) (hT : 0 < T) :
C kappa T = Cost.Jcost (turnRatio kappa T) :=
censusPricing_of_anomalyLedger C h kappa T hk hT
What this page does not claim
The theorem does not identify κ with any physical horizon clock rate. The theorem does not prove that the anomaly reading is the only possible reading. The theorem does not assert that the physical seam cost satisfies the ledger closure condition.
Verify this page
Every tagged claim above names its theorem. To check one yourself rather than trust this page, elaborate the source module with Lean 4 and audit its axiom basis:
$ lake env lean IndisputableMonolith/Holography/SeamLedgerDischarge.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
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Derived articles
This page is generated by a question-recursion engine: the questions its answers raise become the next pages. The current agenda, with open targets marked red:
- What physical system, if any, satisfies the ledger closure pricing condition?
- How is the rate parameter κ identified with a physical horizon's clock rate?
- Does the deficit-free period 2π/κ appear in any measured physical phenomenon?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM b2_unique_zero_of_anomalyLedger · IndisputableMonolith/Holography/SeamLedgerDischarge.lean
/-- **B2 through the landed chain (THEOREM, CITED).** At the anomaly reading the B2 discharge also follows from `b2_unique_zero_of_conserving` — consistency check that the weak route and the landed route agree on the zero set. -/ theorem b2_unique_zero_of_anomalyLedger (C : ℝ → ℝ → ℝ) (h : LedgerClosurePricing anomalyReading C) (kappa T : ℝ) (hk : 0 < kappa) (hT : 0 < T) : C kappa T = 0 ↔ T = DeficitFreePeriod.euclideanPeriod kappa := b2_unique_zero_of_conserving C (conservingSeamPricing_of_anomalyLedger C h) kappa T hk hTfor any positive rate parameter κ and any positive period T, the cost C(κ, T) equals zero if and only if T equals 2π/κ b2_unique_zero_of_anomalyLedger · IndisputableMonolith/Holography/SeamLedgerDischarge.leanTHEOREM conserving_trace_bound · IndisputableMonolith/Holography/SeamLedgerDischarge.lean
/-- **The key new lemma, bundled (THEOREM):** for pairing-conserving `W` with real eigenvalue `x > 0`, `Tr W = x + x⁻¹ ≥ 2`, with equality iff `x = 1`. This is what lets the discharge below run on ANY calibrated faithful trace reading, not just the character anomaly: the trace separates "deficit-free" from "mismatched" all by itself. -/ theorem conserving_trace_bound {W : Matrix (Fin 2) (Fin 2) ℝ} {x : ℝ} (hcons : ∀ u v, pairForm (W.mulVec u) (W.mulVec v) = pairForm u v) (hx : 0 < x) (h : HasRealEigen W x) : W.trace = x + x⁻¹ ∧ 2 ≤ W.trace ∧ (W.trace = 2 ↔ x = 1) := ⟨conserving_trace_eq hcons hx h, conserving_trace_ge_two hcons hx h, conserving_trace_eq_two_iff hcons hx h⟩for such a matrix W with a positive real eigenvalue x, its trace equals x + x⁻¹, which is always at least 2, with equality exactly when x = 1 conserving_trace_bound · IndisputableMonolith/Holography/SeamLedgerDischarge.leanTHEOREM b2_unique_zero_of_ledgerClosure · IndisputableMonolith/Holography/SeamLedgerDischarge.lean
/-- **B2 from the weak residue (THEOREM, FORCED-CONDITIONAL on `LedgerClosurePricing`).** For ANY calibrated faithful trace reading, the deficit-free period `β = 2π/κ` is the UNIQUE zero of the per-cycle cost: * off the period, `turnRatio ≠ 1` (`turnRatio_eq_one_iff`, CITED), so the trace is strictly above 2 (`conserving_trace_bound`) and faithfulness forbids a zero; * at the period, `turnRatio = 1`, the trace is exactly 2, and calibration fires. The character anomaly appears NOWHERE: the B2 zero set is forced by conservation, delivery, calibration, and faithfulness alone. -/ theorem b2_unique_zero_of_ledgerClosure (R : TraceReading) (C : ℝ → ℝ → ℝ) (h : LedgerClosurePricing R C) (kappa T : ℝ) (hk : 0 < kappa) (hT : 0 < T) : C kappa T = 0 ↔ T = DeficitFreePeriod.euclideanPeriod kappa := by obtain ⟨W, hcons, heig, hC⟩ := h kappa T hk hT have hx : 0 < turnRatio kappa T := turnRatio_pos hk hT rw [hC] constructor · intro h0 by_contra hne have hx1 : turnRatio kappa T ≠ 1 := fun h1 => hne ((turnRatio_eq_one_iff kappa T hk).mp h1) have htr2 : W.trace ≠ 2 := fun heq => hx1 ((conserving_trace_eq_two_iff hcons hx heig).mp heq) have hgt : 2 < W.trace := lt_of_le_of_ne (conserving_trace_ge_two hcons hx heig) (Ne.symm htr2) exact R.faithful W.trace hgt h0 · intro hTeq have hx1 : turnRatio kappa T = 1 := (turnRatio_eq_one_iff kappa T hk).mpr hTeq have htr : W.trace = 2 := by rw [conserving_trace_eq hcons hx heig, hx1] norm_num rw [htr] exact R.calibratedthe same conclusion follows for any reading function satisfying those two conditions b2_unique_zero_of_ledgerClosure · IndisputableMonolith/Holography/SeamLedgerDischarge.leanTHEOREM cost_eq_J_of_anomalyLedger · IndisputableMonolith/Holography/SeamLedgerDischarge.lean
/-- **The cost is J of the turn ratio (THEOREM, FORCED-CONDITIONAL).** At the anomaly reading, the weak premise forces `C κ T = J(κT/2π)` — the full T5 pricing, recovered by citation of the landed chain. -/ theorem cost_eq_J_of_anomalyLedger (C : ℝ → ℝ → ℝ) (h : LedgerClosurePricing anomalyReading C) (kappa T : ℝ) (hk : 0 < kappa) (hT : 0 < T) : C kappa T = Cost.Jcost (turnRatio kappa T) := censusPricing_of_anomalyLedger C h kappa T hk hTthe cost function equals the framework's canonical cost J(x) = (x + 1/x)/2 − 1 cost_eq_J_of_anomalyLedger · IndisputableMonolith/Holography/SeamLedgerDischarge.lean