Established within the stated premises
Given two-face source yields opposite neutral Weyls and bounded time reflection
finding:given-two-face-source-derives-opposite-neutral-weyls-and-bounded-time-reflection
The old Schottky reflection rho(t,s)=(-t,s) does not reverse spatial profiles; its neutral Weyl profile map is -I and is not excluded by the previous -r_s result. In the existing HS source space, W_R(f)=L_Wf and W_L(f)=R_Wf* have opposite Weyl phases directly from right multiplication. J_HS W_R J_HS=W_L is conjugate-linear multiplicative; centered finite bilinears obey j_L(A)=-R_j(A) and J n_R J=I-n_L. The joint functional Tr(sqrt(rho)Wi*sqrt(rho)Wj) is the positive HS Gram of rho^1/4 Wi rho^1/4 without a Gaussian premise. For the given thermal source, fully ordered heat products K_F handle bounded even insertions: ||K_F||2<=sqrt(Z_beta)product||Aj|| and S(ThetaF,G)=Tr K_F* K_G/Z_beta. Strong approximation extends the existing polynomial free functional to existing bounded neutral Weyls. The old Green midpoint X and all four graph blocks are reused, not chosen anew. Exact NS modes pi,3pi test the same original implementation path, including null relations, particle-hole contribution and reflected noncommuting histories.
Scope: Analytic all-mode theorem in the explicitly existing normal source representation, supplemented by exact finite path controls, not an all-mode inference from finite samples. W(f) must already be bounded in the source von Neumann algebra; no norm CAR membership, bounded imaginary-time conjugates or arbitrary odd OS words asserted. The GNS partner is not identified with a physical P1 second boundary. Older papers32 and45 assume the positive field kernel or its reflection positivity. Actual local physical P1 source map, original measure/coupling, physical time, EM and complete TFPT remain open. The old spatial type exclusion retains its stated scope.
Required premises and original source excerpts
- Do not identify source types
Observable algebra, OS reflection, state, collar operator, time evolution, carrier connection, family holonomy, and readout are distinct data until an original map relates them.
premise:typed-source-structures - Normal even sea CAR source with canonical graded HS doubling
For the algebraic source test use the already given sea Fock/CAR carrier,with faithful even normalized traceclass density rho and its standard HS space,Omega=sqrt(rho),L_A X=AX,R_A X=XA,Gamma X=Pi X Pi. Gamma is the canonical GNS implementer of source parity fixing Omega. Partner fields are represented in the fixed mode-index chart by b_j=−Gamma R_aj;this assumes no physical second P1 boundary. The finite saturation theorem covers arbitrary faithful even finite densities;the separate all-mode route requires the actual normal HS carrier,a complete covariance eigenbasis and saturation in every mode. For the free elliptic connection,rho is the already derived original thermal density,not a newly chosen geometry or temperature. TomitaJ,OSTheta,classical doubling and physical time remain distinct until actually mapped.
premise:normal-even-sea-car-source-and-canonical-graded-hs-double - Free chiral Cauchy quantization of the canonical elliptic annulus
Treat the dividing half of the given square curve in its canonical flat conformal representative as a product collar. Compute the Cauchy graph of Dplus=partial_t+B_Sigma,B_Sigma=−i partial_s with NS boundary,then interpret it using the expressly free chiral CAR construction as a quasifree two-boundary state. The labelled second-face compression is the covariance;the other is complementary. This Gaussian interpretation does not derive the original relative spectral-action measure,P1 time or EM/Quillen response.
premise:free-chiral-cauchy-quantization-of-canonical-elliptic-annulus - Existing normal thermal source with bounded neutral insertions
Use the already given thermal sea representation of the free elliptic NS source with H>=0, finite Z_beta=Tr exp(-beta H), W=beta/2, rho=exp(-beta H)/Z and its HS standard space. Neutral even insertions including existing current Weyls are bounded in the source von Neumann algebra. Their imaginary-time conjugates are not assumed everywhere bounded; ordered heat products define the functional. The general HS Gram formula needs only an existing normal density, not Gaussianity. This comparison premise asserts neither physical P1 source, second geometric field family nor physical time identification.
premise:existing-normal-thermal-source-with-bounded-neutral-insertions
- experiments/theory-contracts/elliptic-moebius-source-bridge-20261026/two_face_source_20261029/PROOF.txt, lines 1–185
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- documents/archive--tfpt-45--source_extracts--04_qft_source/sections/002-section-closure-theorems-from-the-admissibility-complex.tex, lines 256–310
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