TFPT scientific source excerpt Original repository path: experiments/theory-contracts/seam-joint-source-origin-audit-20261016/PROOF.txt Original file SHA-256: f91443b115994302aa3b10d2a6b44131e13c3998b13d47b34aeaa59e25c86315 Inclusive original lines: 52-82 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. 000052 | 3. First attempted bridge: determinant class -> positive carrier rank 000053 | 000054 | Let S2 denote _archive/tfpt-45/source_extracts/02_carrier_source.tex. 000055 | Its determinant-class theorem starts at1894 and already uses 000056 | X=-2P3+3P2 (1908; repeated1938) 000057 | and the explicitly named weak rank-two sector (1936-1944). 000058 | Its compact-index theorem then uses L2=det E2=O(1), and the rank-two corollary 000059 | (2075-2095) infers dim E_plus=2 from H^0(P1,O(1))=C^2. 000060 | This is conditional reuse of the closed branch, not an independent upstream 000061 | derivation of that branch. The later carrier-rigidity proof calls this corollary. 000062 | 000063 | There is also a concrete object-type gap. The dimension of the space of global 000064 | sections of a determinant LINE is not the fiber rank of the underlying bundle: 000065 | F_r=O(1) direct_sum O(0)^(r-1) 000066 | has det F_r=O(1) for every r>=1, but rank F_r=r and h0(F_r)=r+1. 000067 | At fixed rank2 and determinant degree1, O(1)+O(0) has (h0,h1)=(3,0), 000068 | whereas O(3)+O(-2) has (h0,h1)=(4,1). Thus determinant degree does not fix 000069 | even the kernel of an arbitrary bundle Dolbeault operator at fixed rank. 000070 | These are elementary bundle controls, not alternative physical TFPT worlds. 000071 | 000072 | The source must supply the actual bosonic operator, its bundle and its 000073 | equivariant identification with the desired internal carrier. The numerical 000074 | identity h0(O(1))=2 cannot substitute for this map. Likewise a geometric 000075 | rotation action on sections cannot silently be identified with weak gauge action. 000076 | The stated analytic index must retain its operator and normalization: chi(O(1))=2; 000077 | counting one doublet is not automatically that same Fredholm index. 000078 | 000079 | The Lean HiggsIndexCertificate explicitly assumes 000080 | toForms : Eplus equiv_linear DegreeOneBinaryForms. 000081 | Its dimension theorem is valid under this premise. This audit does not refute it 000082 | and does not claim a new Lean build.