TFPT scientific source excerpt Original repository path: experiments/theory-contracts/tfpt-unified-source-derivation-20261029/aps_source_review/DYNAMICAL-HIGGS-SOURCE-PROOF.txt Original file SHA-256: eda5bb664b1fb20370e59b39dbd5e3cb04d79864a8d1d0a0eb6c791cdaf98f49 Inclusive original lines: 109-139 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. 000109 | truncation or a substitute boson measure. The complex H2 coefficient is also 000110 | checked directly in the existing joint_source exterior algebra. 000111 | 000112 | 4. Fermion-first evaluation, determinant and mixed correlations 000113 | 000114 | The full source can also be evaluated by integrating fermions first. For a 000115 | fixed background H in an actually specified bilinear charged chart it gives 000116 | the unnormalized Berezin polynomial P_H[eta,bar eta], including det K[H]. 000117 | On the invertible chart only, 000118 | P_H=det K[H] exp(bar eta K[H]^-1 eta), 000119 | with the original Berezin orientation. Coefficients are complementary minors 000120 | and extend polynomially through singular K; do not discard zero-determinant 000121 | fibers that still carry nonzero sourced coefficients. Actual Majorana/chiral 000122 | blocks require the actual skew pairing and Pfaffian instead. 000123 | 000124 | Reuse the established same-collar skew pairing 000125 | [[0,-Lplus^t],[Lplus,0]] 000126 | whose Pfaffian is (-1)^(n(n+1)/2)det Lplus at finite n. The orientation fixes 000127 | this sign. One must not integrate all96 doubled internal labels again as 000128 | independent physical complex fermions, square the determinant, replace a 000129 | Pfaffian by abs(det) or infer the physical chiral restriction from96 alone. 000130 | This kinetic/KO distinction was already established and is reused. Primary 000131 | context: Chamseddine,Connes,Marcolli hep-th/0610241, section4,especially4.4.1. 000132 | 000133 | When the actual fixed-H fibers are Gaussian, the two- and four-point source 000134 | coefficients of their common integral are weighted averages of C_H and of 000135 | C_H,ij C_H,kl-C_H,il C_H,kj, respectively. Subtracting the Wick expression 000136 | of the averaged C gives the difference of two weighted covariances. Use the 000137 | actual det/Pf-weighted functional, not the bare boson measure, and only divide 000138 | where its scalar is nonzero. Signed/complex weights are not probabilities. 000139 | Variation of C_H generically yields a non-Gaussian marginal, but neither H