TFPT scientific source excerpt Original repository path: experiments/theory-contracts/tfpt-unified-source-derivation-20261029/aps_source_review/ORIGINAL-HIGGS-INNER-SCALE-PROOF.txt Original file SHA-256: 8d041b0da6aef4a5e90007fb4c155029133138097e895517b396cb4fee32ef58 Inclusive original lines: 171-198 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. 000171 | constant-dimensional kernel, and its stated scale operation really is fBf 000172 | with the transported domain. This assumption is not inferred from its index. 000173 | Let S:C^k -> kerB be the given isometric basis map. Then 000174 | ker(fBf)=f^-1 kerB, 000175 | G=S* f^-2 S>0, T=f^-1 S G^-1/2, 000176 | T*T=I, rangeT=ker(fBf). (8) 000177 | For an ACTUAL vertex X whose relevant mode vectors are in its domain, 000178 | T*(fXf)T=G^-1/2 S*XS G^-1/2, 000179 | T*X T=G^-1/2 S*f^-1Xf^-1 S G^-1/2. (9) 000180 | No scalar exponent is assumed: G need not be diagonal or scalar if f varies 000181 | across the normal fiber. These are full matrix identities. For q=f² constant 000182 | ON that fiber, G=q^-1I and T=S in the same original Hilbert metric. 000183 | The overlaps then scale by q for fXf, and by1 for X. Mode normalization 000184 | alone does not choose which vertex the original inserts. 000185 | 000186 | For the given k=2 COMPLEX mode coefficients, h_norm=G^1/2 H_raw, hence 000187 | d4H_raw=(det_C G)^-1 d4h_norm (10) 000188 | when that coefficient measure is flat. This is a DIFFERENT change from(5), 000189 | whose Jacobian is q^4. Do not confuse normalized mode coordinates, the affine 000190 | seed coordinate, and the conformally transformed physical Higgs field qH. 000191 | Use the pushforward for a non-flat original measure. For x-dependent modes 000192 | retain the induced connection T*nabla T and exterior derivative couplings; 000193 | the exact Schur/memory response is not discarded by retaining only zero modes. 000194 | No actual normal metric, profile or overlap insertion is chosen here. 000195 | Isolation of the zero eigenvalue is required for the usual smooth spectral 000196 | projection perturbation theorem, not for the pointwise algebraic kernel 000197 | identity(8). No extra isolation gate is imposed on that identity. 000198 |