Established in scope
Finite SM Higgs fluctuation retains the supplied Yukawa seed
In the question: Historical: common source, state and event selection
Exact conditional classification of the particle LR block of the given representation, not a complete real-triple classification or P1/P2-derived coupling. Already encoded3+2 structure is not newly selected.
Read the exact result, assumptions and evidence
Result
For M=diag(Yup,Ydown), every particle LR one-form obeys q_a(Mr_b−q_bM)=q_a(r_b−q_b)M. The factor is quaternionic and b=eR spans all qM. Including the seed yields M(H)=HM with H=[[φ1,φ2],[-barφ2,barφ1]]. The four Yukawa matrices and color/weak modules remain inputs; D_F=0 gives no finite fluctuation. The linear identity was checked exactly against unchanged existing code with a complete coefficient basis, without choosing physical couplings.
Required assumptions
- Given finite SM representation with symbolic Yukawa inputs
Use only the existing v252/v254 representation with C⊕H⊕M3, already supplied color/weak modules and four symbolic complex3×3 Yukawa blocks. No physical values are chosen or fitted. Classify the particle LR one-form block; no proof of the full real96-dimensional fluctuation with antiparticles, JAJ and Majorana sector is claimed.
- Do not identify source types
Observable algebra, OS reflection, state, collar operator, time evolution, carrier connection, family holonomy, and readout are distinct data until an original map relates them.
Original evidence
- HIGGS_VARIATION_PROOF.txt lines 135–182
Source checked at this snapshot
Original location and fingerprint
experiments/theory-contracts/seam-joint-source-origin-audit-20261016/HIGGS_VARIATION_PROOF.txt
84004fc583641a52096c8571844aaed825d16d8165635eafd1a6b2562708e6be
finding:finite-sm-higgs-variation-retains-seed