TFPT scientific source excerpt Original repository path: experiments/theory-contracts/original-admissible-source-closure-20261025/KMS-AND-CARRIER-TRANSPORT.txt Original file SHA-256: 9efcfb0d68e16db842aab97b7171b2d667e7b065cb4c6ab8138102acc4c8fb68 Inclusive original lines: 241-286 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. 000241 | 9. Real EM response, phases, and the reference sector 000242 | ----------------------------------------------------- 000243 | 000244 | For the literal reflected covariance I-C, the same winding gives the inverse 000245 | factor (1-z)^(-1). The ordinary full relative pair, and the norm of THAT 000246 | inverse pair, are therefore one. Taking a square root of that norm cannot 000247 | produce 1-z. A positive pair with determinant (1-z)^2 would be a different 000248 | operator and needs an original source identity. 000249 | 000250 | This does not say that a full Dirac field has zero real EM susceptibility. 000251 | Its actual D_A*D_A determinant is a different object. The even spectral 000252 | action, eta phase, and the chiral determinant line must remain typed. 000253 | 000254 | The inverse-pair result is a scoped control, not an imposed physical source: 000255 | v42 starts with the labeled one-sided datum (A_+,H_+,D_+,B_Sigma), and its 000256 | minimal EM transfer contains no reflected inverse partner. Nevertheless 000257 | tr_adm lives on Ran(P_adm) inside H_OS; the source does not identify it with 000258 | the labeled graph marginal used in section4. Neither P_C nor Gamma supplies 000259 | that face selection. A new chiral measure is therefore not imposed as a 000260 | prerequisite for the real EM response. The required equality is the actual 000261 | state/time-preserving one-sided source map and its response functional. 000262 | 000263 | Let b=B gamma=5/4 and q(alpha)=delta_top exp(-2 alpha), as in the originals. 000264 | The current operator theorem proves the candidate 000265 | 000266 | -b Log det_F R_C(q(alpha))=-b Log(1-q(alpha)). (12) 000267 | 000268 | The exponent b and the identification with the physical EM effective action 000269 | are not derived by (1). A sufficient actual Dirac-source comparison is 000270 | 000271 | Re[Gamma_F(alpha)-Gamma_F(alpha_*)] 000272 | =-(1/2)log det_rel^+(D_alpha^*D_alpha,D_*^*D_*) 000273 | =-b log[(1-q(alpha))/(1-q(alpha_*))]. (13) 000274 | 000275 | Here D_*=D_(alpha_*). 000276 | The symbol det_rel^+ denotes a properly defined positive RELATIVE 000277 | determinant with the original local counterterms/regularization retained; 000278 | no multiplicativity of arbitrary separate zeta determinants is assumed. 000279 | The reference alpha_* must be stated. In particular q(0)=delta_top is NOT 000280 | zero. A seam-free reference q_ref=0 is a different reference, and must be 000281 | named as such. The holomorphic branch is Log(1)=0 on |z|<1. 000282 | 000283 | The old complete-sector criterion R(alpha)=R(alpha_*) remains necessary 000284 | when the rest of the source is integrated out. The Schur-complement identity 000285 | does not prove that residual ratio constant or remove a genuine source 000286 | normalization term.