TFPT scientific source excerpt Original repository path: documents/archive--paper-latex--tfpt-42/sections/006-subsection-character-trace-identities-and-the-abelian-in.tex Original file SHA-256: 341f53fab64f6f2cca53e505d497cdc7087285c95e8e0f44f616ac6754afa810 Inclusive original lines: 131-170 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. 000131 | moments of $X$. 000132 | \end{proof} 000133 | 000134 | \begin{remark}[Table as readout, character as proof device] 000135 | The one-family table remains useful as a reader-facing decoding sheet, but the whole six-sector 000136 | arithmetic is already compressed into the single multiplicative character 000137 | \Cref{eq:multiplicative-family-character}. 000138 | \end{remark} 000139 | 000140 | \begin{remark}[Six admissible occupancy sectors] 000141 | The six monomials in \Cref{eq:split-weight-enumerator} are exactly the six allowed occupancy pairs $(n_3,n_2)$ of the family packet. This is the shortest combinatorial route from the split carrier to the six Standard Model multiplet sectors listed in \Cref{tab:one-family}. 000142 | \end{remark} 000143 | 000144 | The carrier packet therefore reproduces the standard trace cancellations 000145 | \[ 000146 | \tr_{S^+}Y=0, 000147 | \qquad 000148 | \tr_{S^+}Y^3=0, 000149 | \] 000150 | and packages them together with the quadratic trace in one formula. Since $\tr_{S^+}Y^2=4\gamma=10/3$ and $\tr_\Phi Y^2=1/2$ for one weak doublet with hypercharge $1/2$, the hypercharge trace coefficient organizes as 000151 | \begin{equation} 000152 | \label{eq:abelian-index} 000153 | \bone(N_{\mathrm{fam}},N_\Phi) 000154 | = 000155 | \frac25N_{\mathrm{fam}}\tr_{S^+}Y^2+\frac15N_\Phi\tr_\Phi Y^2 000156 | = 000157 | \frac85N_{\mathrm{fam}}\gamma+\frac1{10}N_\Phi 000158 | = 000159 | \frac43N_{\mathrm{fam}}+\frac1{10}N_\Phi. 000160 | \end{equation} 000161 | On the canonical branch $(N_{\mathrm{fam}},N_\Phi)=(3,1)$ this gives 000162 | \[ 000163 | \bone=\frac{41}{10}. 000164 | \] 000165 | The abelian index is therefore not inserted as an isolated Standard Model datum; it is a carrier-level output once the family and Higgs counts are declared. 000166 | 000167 | \begin{remark}[Canonical-branch Diophantine lock] 000168 | If one imposes $\bone=41/10$ on nonnegative integer data, then 000169 | \[ 000170 | 40N_{\mathrm{fam}}+3N_\Phi=123.