TFPT scientific source excerpt Original repository path: experiments/theory-contracts/native-arc-charge-source-interface-20261026/PROJECTOR-STATE-REVIEW.txt Original file SHA-256: 4b9abbcb3b3f0dcf9a99a4ec09640b28aaa938d1f78b47cc409cc89f81aaf934 Inclusive original lines: 1-72 Line numbers below refer to the original source. This bounded excerpt is source evidence; it is not a new proof/checker run. Conversation metadata and personal execution details are omitted where indicated. 000001 | Independent scoped mathematical review 000002 | 26 October 2026 000003 | 000004 | Claim: UR.NATIVE.ARCCHARGE.PROJECTOR-STATE.01 000005 | Verdict: ACCEPT_EXACT_STATED_SCOPE. No material correction required. 000006 | 000007 | Read PROJECTOR-STATE-RIGIDITY.txt and check_projector_state_rigidity.py fully. 000008 | Directly checked Araki, On Quasifree States of CAR and Bogoliubov 000009 | Automorphisms, Publ.RIMS6(1970/71), Lemma4.3 and Definition4.4: 000010 | https://ems.press/content/serial-article-files/41673?nt=1 000011 | Lemma4.3 assumes an arbitrary state with the required annihilator null norms, 000012 | not an already quasifree state. It therefore supports the claimed removal 000013 | of an independent Gaussian premise once the full projector covariance of a 000014 | positive CAR state is actually known. 000015 | 000016 | 1. Exact uniqueness 000017 | GNS positivity gives a(f)Omega=0 on kerP and a*(f)Omega=0 on ranP. 000018 | CAR normal ordering then determines every finite polynomial expectation; 000019 | norm density extends uniqueness to the CAR C* algebra. Gauge invariance, 000020 | vanishing anomalous pairs and Wick factorization follow, rather than being 000021 | assumed. The text correctly distinguishes infinite CAR/GNS uniqueness from 000022 | implementability in a separately chosen representation or existence of a 000023 | global density matrix in that representation. 000024 | 000025 | 2. Original annulus source and missing physical equation 000026 | The actual closed graph gives the bounded full projector with diagonal 000027 | blocks I-C_A,C_A and offdiagonal X_A=(2cosh(W B_Sigma))^-1. 000028 | The functional-calculus identity X_A^2=C_A(I-C_A) verifies idempotence. 000029 | The text does not treat the unbounded exponential transfer as an everywhere 000030 | defined bounded map. A single face covariance is explicitly not a projector. 000031 | The physical conclusion is correctly conditional on an actual joint charged 000032 | CAR embedding and the complete measured/derived covariance, especially 000033 | omega_P1(a_L*(f)a_R(g))=. This equation is not obtained by choosing 000034 | a purification of C_A. The original labelled chiral scalar source is kept 000035 | distinct from a full Dirac vector source, normal Clifford action, OS 000036 | admissibility and physical time. 000037 | 000038 | 3. Quantitative finite block 000039 | On a finite genuinely P-reducing block, Q_P has a unique Slater zero vector 000040 | and a unit excitation gap. Hence Q_P>=I-rho_P, the displayed trace formula 000041 | for delta is correct for arbitrary positive states, and the pure-target 000042 | trace-distance bound gives ||rho-rho_P||_1<=2sqrt(delta). 000043 | Bounded-word error estimates apply only to that block. Spatial or one-face 000044 | compressions cannot silently replace a reducing block. The coherent, 000045 | dephased and product controls have the stated equal marginals and distinct 000046 | cross correlations/four-point values. The coherence defect formula is correct. 000047 | 000048 | 4. Positive ensembles 000049 | The extreme-projection argument is valid for normalized positive ensembles 000050 | with the stated separability/measurability scope. A countable dense set in 000051 | the empty and filled subspaces suffices; positivity forces the remaining 000052 | offdiagonal entries as well. Signed or complex weights are correctly kept 000053 | outside this ensemble argument. No primitive P1 measure is thereby derived. 000054 | 000055 | 5. Independent replay 000056 | Ran python3 -B check_projector_state_rigidity.py and python3 -B -OO 000057 | check_projector_state_rigidity.py, without output paths. Both exited0 and 000058 | returned the stored result, including all256 ordered four-field words, 000059 | excitation spectrum0^1,1^2,2^1 and the non-Gaussian marginal controls. 000060 | RuntimeError checks remain active. These finite checks are not substituted 000061 | for the all-degree GNS proof. Only this review file was written. 000062 | 000063 | Reviewed SHA256: 000064 | PROJECTOR-STATE-RIGIDITY.txt 000065 | 2e14e8875c263d71bd6bda61d005461cb718bdf30fdf34a6312db53167cd80c6 000066 | check_projector_state_rigidity.py 000067 | 8439a30ad767f138f9269aa2bc6beca1f2d3d7088e92862bcd76fbf40d5a7c16 000068 | projector_state_rigidity_results.json 000069 | 40737f35ef6967cdfa2742f5f79d722f677a1adbb5a3770b9b0ee12bd190fe75 000070 | 000071 | Experiment-only application of known CAR rigidity. No primitive source, 000072 | interaction, spacetime, empirical or ledger promotion is implied.