TFPT scientific source excerpt Original repository path: documents/archive--tfpt-45--source_extracts--02_carrier_source/sections/001-subsection-carrier-algebraic-normal-form.tex Original file SHA-256: fb846ac340cc9f8ea0aa6431598b624f2f744fa08b7d4cfdc081c358d1ea7cee Inclusive original lines: 172-283 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. 000172 | Hence from now on 000173 | \[ 000174 | E=E_3\oplus E_2, 000175 | \qquad 000176 | X=-2P_3+3P_2, 000177 | \qquad 000178 | P_3=\frac{\mathbf 1-\epscar}{2}, 000179 | \qquad 000180 | P_2=\frac{\mathbf 1+\epscar}{2}, 000181 | \] 000182 | and the hypercharge operator is the normalized primitive two-point generator 000183 | \begin{equation} 000184 | \label{eq:explicit-hypercharge} 000185 | Y 000186 | = 000187 | \mathrm{diag}\!\left(-\frac13,-\frac13,-\frac13,\frac12,\frac12\right) 000188 | = 000189 | \frac{X}{6} 000190 | = 000191 | -\frac13 P_3+\frac12 P_2 000192 | = 000193 | \frac1{12}\mathbf 1+\frac5{12}\epscar. 000194 | \end{equation} 000195 | 000196 | \begin{lemma}[Charge-generator / carrier-polarization inversion] 000197 | On the rigid carrier, the carrier polarization and the primitive two-point generator are recovered by 000198 | \begin{align} 000199 | \epscar&=\frac{2X-\mathbf 1}{5}=\frac{12Y-\mathbf 1}{5}, 000200 | \label{eq:hypercharge-seam-inversion}\\ 000201 | \qquad 000202 | X&=\frac{5\epscar+\mathbf 1}{2}, 000203 | \nonumber\\ 000204 | (2X-\mathbf 1)^2&=25\,\mathbf 1, 000205 | \nonumber\\ 000206 | X^2-X-6\,\mathbf 1&=0, 000207 | \nonumber\\ 000208 | 6Y^2-Y-\mathbf 1&=0. 000209 | \label{eq:carrier-polynomial} 000210 | \end{align} 000211 | Consequently the carrier projectors are 000212 | \[ 000213 | P_2=\frac{\mathbf 1+\epscar}{2}=\frac{2(3Y+\mathbf 1)}{5}, 000214 | \qquad 000215 | P_3=\frac{\mathbf 1-\epscar}{2}=\frac{3(\mathbf 1-2Y)}{5}. 000216 | \] 000217 | \end{lemma} 000218 | 000219 | \begin{proof} 000220 | The affine relations between $(X,Y)$ and $\epscar$ are inverted algebraically. Squaring the first 000221 | relation and using $\epscar^2=\mathbf 1$ gives the quadratic generator polynomial 000222 | $X^2-X-6\,\mathbf 1=0$, and dividing by $36$ yields the hypercharge polynomial. The projector 000223 | formulas then follow from $P_2=(\mathbf 1+\epscar)/2$ and $P_3=(\mathbf 1-\epscar)/2$. 000224 | \end{proof} 000225 | 000226 | \begin{lemma}[Primitive trace-balanced carrier] 000227 | \label{lem:primitive-trace-balanced-carrier} 000228 | Let $Y$ be an endomorphism of a finite-dimensional carrier $E$ such that 000229 | \[ 000230 | 6Y^2-Y-\mathbf 1=0, 000231 | \qquad 000232 | \tr_EY=0, 000233 | \] 000234 | and assume the realization is primitive in the sense that $E$ is not a nontrivial direct sum of 000235 | identical trace-balanced $Y$-modules. Then 000236 | \[ 000237 | \operatorname{Spec}(Y)=\left\{-\frac13,\frac12\right\}, 000238 | \qquad 000239 | \dim\ker\!\left(Y+\frac13\mathbf 1\right)=3, 000240 | \qquad 000241 | \dim\ker\!\left(Y-\frac12\mathbf 1\right)=2. 000242 | \] 000243 | Equivalently, 000244 | \[ 000245 | \rank E=5, 000246 | \qquad 000247 | E=E_3\oplus E_2, 000248 | \qquad 000249 | Y=-\frac13P_3+\frac12P_2. 000250 | \] 000251 | \end{lemma} 000252 | 000253 | \begin{proof} 000254 | The quadratic polynomial factors as 000255 | \[ 000256 | (2Y-\mathbf 1)(3Y+\mathbf 1)=0, 000257 | \] 000258 | so the only eigenvalues are 000259 | \[ 000260 | y_+=\frac12, 000261 | \qquad 000262 | y_-=-\frac13. 000263 | \] 000264 | Write 000265 | \[ 000266 | m_+:=\dim\ker(Y-y_+\mathbf 1), 000267 | \qquad 000268 | m_-:=\dim\ker(Y-y_-\mathbf 1). 000269 | \] 000270 | Then 000271 | \[ 000272 | 0=\tr_EY=\frac12\,m_+-\frac13\,m_-, 000273 | \] 000274 | so 000275 | \[ 000276 | 3m_+=2m_-. 000277 | \] 000278 | Because $\gcd(2,3)=1$, every positive integer solution has the form 000279 | \[ 000280 | (m_+,m_-)=(2k,3k). 000281 | \] 000282 | Primitivity forces $k=1$, hence $(m_+,m_-)=(2,3)$. This is exactly the rigid $3+2$ split, with 000283 | the displayed spectral form of $Y$.