TFPT scientific source excerpt Original repository path: experiments/theory-contracts/original-admissible-source-closure-20261025/P1-W8-LOCAL-MAP-AND-TWOPOINT-TEST.txt Original file SHA-256: 072b6588666504ec4f04024e279030bbdf83b724102bac181ee3696133c1be28 Inclusive original lines: 174-197 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. 000174 | 7. Information retained and information the test cannot select 000175 | --------------------------------------------------------------- 000176 | The actual orthogonal root automorphism g=-M R M^-1, with R coordinate 000177 | reversal, takes d_(1/4) to d_(3/4), fixes W8 and preserves N. It intertwines 000178 | the Heisenberg Fock representations of these two real charge modules. 000179 | Therefore ALL separated pure W8 correlation functions in the two charge 000180 | states agree, not merely (4). This does not identify charged CAR fields, 000181 | the full marked clock tuple or their geometric P1 supports. A W8-only test 000182 | cannot choose between these two quarter labels. 000183 | 000184 | At the same time the source is not an exact finite-state dynamics. For 000185 | every ell>=1, the convergent expansion of (6) has 000186 | 000187 | a_ell=sum_(r=1)^min(ell,8) binom(ell+r-1,2r-1)A_r 000188 | >=ell A1>0. (7) 000189 | 000190 | Hence infinitely many distinct N levels occur. To avoid any point-field 000191 | domain issue, apply the existing positive semigroup e^(-epsilon N) to the 000192 | one-insertion vector. Its spectral coefficients become 000193 | a_ell exp(-2epsilon ell)>0 and its norm is finite for every epsilon>0. 000194 | The cyclic time subspace is still infinite dimensional. No finite spectral 000195 | support with this same time generator can reproduce its exact two-point 000196 | function. Finite approximations and finite native observation codes remain 000197 | possible; they are not the complete local source dynamics.