TFPT scientific source excerpt Original repository path: experiments/theory-contracts/tfpt-unified-source-derivation-20261029/aps_source_review/ORIGINAL-HIGGS-FIBER-PROOF.txt Original file SHA-256: 67be41084a14e3934cbb2c743f3969c0443e5b9180b2f4cdeeed5a884d566a5e Inclusive original lines: 1-43 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. 000001 | ORIGINAL HIGGS FIBER: WHOLE96 ORBIT, DETERMINANT JET AND RESIDUE MATCH 000002 | 31 October2026. Results R028/R029. Established scoped algebra; source-match 000003 | failure of specific printed formulas. No physical completion or ledger change. 000004 | 000005 | 1. Question and original data 000006 | Continue F1.M6 at its actual source consumer. Keep the original four supplied 000007 | 3x3 matrices Yu,Yd,Ye,Ynu and symmetric MR, weak quaternion q(H), whole96 000008 | particle/antiparticle and chirality slots, and the original source/state maps. 000009 | Do not optimize Yukawas, change primitive profile, add Gamma_H to a master, 000010 | or identify a bare Hessian with the full connected H covariance. 000011 | Original v252 full_D and rep supply the actual coefficients. R026's288 images 000012 | already identify the complete real Higgs one-form. That result is reused. 000013 | The new question is whether all constant H directions require a search, and 000014 | whether the displayed geometric producer actually matches the displayed H 000015 | potential before it is used as the joint H integration weight. 000016 | 000017 | 2. Entire constant H orbit on the actual original coefficient 000018 | Use real coordinates H=(x1+i x2,x3+i x4), u=sum x_a^2 and r=sqrt(u). 000019 | There is no1/sqrt2 factor in these coordinates. The original quaternion is 000020 | q(H)=[[bar h2,h1],[-bar h1,h2]]. 000021 | It obeys q* q=u I2 and det q=u. For r>0, U=q/r lies in SU2. 000022 | Let V(U) act by U on EACH original weak LEFT doublet, identity on all 000023 | right singlets, and complex-conjugate actions on the antiparticle slots. 000024 | Then, with DY=full_D(Yu,Yd,Ye,Ynu,0), DM=full_D(0,0,0,0,MR), 000025 | Phi(H)=V(U) [r DY+DM] V(U)*. (1) 000026 | Proof is the actual LR block multiplication U(r diag(Yup,Ydown)) and its 000027 | adjoint. No commutation with Yup or Ydown is used. DM is between right 000028 | neutrino singlets and remains unchanged. V commutes with original grading 000029 | and JF. At H=0, Phi=DM, so no singular polar coordinate is needed. 000030 | All72 real Y coefficient directions and12 real symmetric MR directions 000031 | are checked against the unmodified original builder at an integral q with 000032 | r=5 using W=rV: W*W=25I and W Phi_rad W*=25 Phi(H), exact integer arithmetic. 000033 | The generic q identities and block proof establish ALL H and ALL matrices; 000034 | one quaternion replay is a constructor check, not the generic proof. 000035 | This is a weak LEFT gauge rotation, not a custodial right symmetry. Unequal 000036 | Yu,Yd or Ynu,Ye do not destroy (1). A contrary Gemini proposal was rejected. 000037 | 000038 | 3. Full determinant reduction, with Majorana and all multiplicities 000039 | For z>0 put P(z,u)=det96(zI+Phi(H)^2). In the original neutrino chiral 000040 | ordering plus=(nuL,antiNuR),minus=(nuR,antiNuL), the whole12 block is 000041 | N=[[0,B],[B*,0]], B=[[r Ynu,0],[MR*,r Ynu^T]], B a6x6 matrix. (2) 000042 | Here * is adjoint; bar is entrywise conjugation. Consequently 000043 | P=det3(z+u Yu*Yu)^12 det3(z+u Yd*Yd)^12