TFPT scientific source excerpt Original repository path: documents/archive--tfpt-45--source_extracts--02_carrier_source/sections/007-subsection-bosonic-relative-index-and-higgs-selection.tex Original file SHA-256: cf801a467465db8d72e4eb3f8e32eea2e23393bf42232a225116c34ed093f761 Inclusive original lines: 185-204 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. 000185 | \[ 000186 | \dim E_+=2. 000187 | \] 000188 | Equivalently, the unique seam-even light bosonic zero mode fills one complex weak doublet and no 000189 | larger positive carrier block is retained. 000190 | \end{corollary} 000191 | 000192 | \begin{proof} 000193 | By \TFPTxref{thm:callias-higgs-selection}, the light seam-even bosonic zero mode lies in the weak block 000194 | \[ 000195 | \Phi\in\Gamma(E_2)\cong (1,2)_{1/2}, 000196 | \] 000197 | and the compact index identifies its zero-mode space with 000198 | \[ 000199 | H^0(S^2,\mathcal O(1))\cong\mathbb C^2. 000200 | \] 000201 | Hence the retained positive carrier block is exactly two-dimensional. 000202 | \end{proof} 000203 | 000204 | This is the sharp form of the Higgs claim used here. The issue is not whether a Higgs doublet can