TFPT scientific source excerpt Original repository path: experiments/theory-contracts/original-admissible-source-closure-20261025/RELATIVE-PAIRING-REVIEW.txt Original file SHA-256: ef280950f70a108ecff5dde9f57c67d097494e3824fdd65aea2ca176b5b83a34 Inclusive original lines: 411-475 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. 000411 | 7. Exact faithful KMS continuation on the existing one-face circle 000412 | ------------------------------------------------------------------- 000413 | 000414 | Let psi_l, l in Z, be the twisted circle basis, 00. 000420 | 000421 | The proposed collar specialization sets beta=2 ell, but the proof is independent 000422 | of that value and holds for every beta>0. Since n_l is strictly decreasing, 000423 | 000424 | D_beta:=u C_beta u^*-C_beta 000425 | 000426 | is diagonal with eigenvalues d_l=n_(l-1)-n_l>0. Moreover 000427 | 000428 | sum_l d_l=lim_(L->infinity)[n_(-L-1)-n_L]=1. (12) 000429 | 000430 | Thus D_beta is positive trace class, Tr D_beta=1. Both C_beta and 000431 | u C_beta u^* are faithful contractions: no eigenvalue is zero or one. For 000432 | |z|<1 the relative operator 000433 | 000434 | R_beta(z)=(I-z u C_beta u^*)(I-z C_beta)^(-1) 000435 | 000436 | differs from the identity by trace class. Its determinant exists, and the 000437 | symmetric finite products telescope: 000438 | 000439 | product_(l=-L)^L (1-z n_(l-1))/(1-z n_l) 000440 | =(1-z n_(-L-1))/(1-z n_L) 000441 | ->1-z. (13) 000442 | 000443 | Trace-norm convergence of the diagonal perturbations justifies passage to the 000444 | Fredholm determinant. Therefore 000445 | 000446 | det_F R_beta(z)=1-z (14) 000447 | 000448 | exactly at every finite beta. As beta tends to infinity, D_beta tends in trace 000449 | norm to the rank-one projector Pi and (14) recovers the pure-sea formula. This 000450 | proves a faithful KMS continuation, not a regularization chosen to fit the 000451 | answer. 000452 | 000453 | The ingredients were already present separately: the actual twisted-circle 000454 | thermal product and source winding are recorded in 000455 | 000456 | experiments/theory-contracts/mixed-current-origin-20261014/ 000457 | ATLAS-KMS-LOCALITY-AND-SOURCE-WINDING.txt:75-121, 000458 | 000459 | and the active source contracts use Fermi-Dirac covariances 000460 | C_beta=(1+exp(beta K))^(-1). The targeted source and Atlas search found no 000461 | previous calculation of the telescoping relative determinant (13). In 000462 | particular, the earlier conclusion that an exact faithful factor 1-z would 000463 | force a rank-one endpoint perturbation applies only to a rank-one compressed 000464 | ansatz; (12)-(14) are its explicit trace-class countercase. 000465 | 000466 | On the reflected face take C_beta^ref=I-C_beta. Then 000467 | 000468 | u C_beta^ref u^*=C_beta^ref-D_beta, 000469 | 000470 | and the same telescoping calculation gives determinant (1-z)^(-1). Hence the 000471 | ordinary full two-face determinant and its Quillen norm remain one. The KMS 000472 | continuation therefore closes only the one-face faithfulness gap. It does not 000473 | select R_pos and does not prove the missing marginal equality (11). Once (11) 000474 | is supplied, the written one-sided EM domain is already the correct type for 000475 | the directed determinant (14).