TFPT scientific source excerpt Original repository path: experiments/theory-contracts/source-localized-spinor-20260919/PROOF.txt Original file SHA-256: 2a08b4d68fc27030cf3e0d2c2e3355b6efa53ad1ed569efee5af059f5691fe02 Inclusive original lines: 121-149 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. 000121 | specified twisted-section convention. It is not a periodic global gauge 000122 | transformation. On the selfdual doubled CAR space use G_a and its conjugate 000123 | on conjugate components; the resulting map respects the CAR real structure. 000124 | 000125 | Cell-averaging G_a f_NS gives exactly Q_N^a(exp(i theta/2)f_NS). 000126 | This defines the source lift L_N of reference test functions. The preceding 000127 | norm and convergence arguments apply componentwise and to their adjoints. 000128 | 000129 | Physical time is retained. On each sourced top-edge charge/oscillator core, 000130 | 000131 | H_a = L0 + (a-1/2)Q, 000132 | 000133 | so at a=1/4 the source time generator is L0-Q/4. The local covariance 000134 | identification does not erase this chemical/holonomy term, choose an E8 000135 | vacuum, or identify its conformal rotations with physical time. 000136 | 000137 | 4. The bounded spinor operation and its source lift 000138 | --------------------------------------------------- 000139 | Primary input: J. Boeckenhauer, Rev. Math. Phys. 8 (1996), Sections 5–7, 000140 | https://arxiv.org/html/hep-th/9507047 . Equations 23–28 give a real 000141 | Bogoliubov unitary V for an even number of Majorana components. Theorem 000142 | 5.4 identifies its restriction to the even vacuum net with a spinor 000143 | sector. This established sector theorem is cited, not re-proved here. 000144 | 000145 | For reproducibility, the operation inside its localization interval can 000146 | be specified pairwise. Write o,e for an odd/even Majorana pair, f_n for 000147 | the interval integer Fourier basis and f_r for its half-integer basis: 000148 | 000149 | V f_0^o = i(f_(1/2)^o-f_(-1/2)^o)/sqrt(2),