TFPT scientific source excerpt Original repository path: documents/archive--tfpt-45--source_extracts--03_em_flavor_source/sections/004-source.tex Original file SHA-256: 107d525221eb816043dbf4fb1a3c7e8244d3e24a5a5bcbfe1c2c34d8ee192f4a Inclusive original lines: 113-163 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. 000113 | \begin{theorem}[Rigid admissible family holonomy class] 000114 | \label{thm:rigid-family-local-system} 000115 | On the rigid four-punctured family section 000116 | \[ 000117 | X_f^\circ\cong \mathbb P^1\setminus\mu_4, 000118 | \] 000119 | fix the determinant line, the local monodromy conjugacy classes at the four punctures, and the 000120 | $D_4$ symmetry inherited from the seam winding theorem. Then there exists a unique admissible 000121 | flat Hermitian family connection 000122 | \[ 000123 | \nabla_F^\star 000124 | \] 000125 | on the flat Hermitian family bundle $L_F\to X_f^\circ$ with fiber 000126 | $F\cong H^1(X_f^\circ,\mathbb C)\cong\mathbb C^3$ whose monodromy representation is the explicit 000127 | holonomy datum $\rho_F$ of 000128 | \TFPTxref{def:canonical-cycle-holonomy,thm:d4-monodromy-rigidity}. Hence its $SU(3)_F$ 000129 | conjugacy class $[\nabla_F^\star]$ is unique. 000130 | \end{theorem} 000131 | 000132 | \begin{proof} 000133 | By \TFPTxref{thm:topological-family-closure}, the family section is the rigid four-punctured sphere 000134 | \[ 000135 | X_f^\circ\cong\mathbb P^1\setminus\mu_4, 000136 | \] 000137 | and it carries the full $D_4$ symmetry inherited from the seam winding data. The determinant line 000138 | is fixed to be trivial, and the local puncture conjugacy classes are fixed by the admissible cusp 000139 | labels. Therefore \TFPTxref{thm:d4-monodromy-rigidity} determines one monodromy representation 000140 | \[ 000141 | \rho_F:\pi_1(X_f^\circ)\to SU(3)_F 000142 | \] 000143 | uniquely up to global $SU(3)_F$ conjugation. 000144 | 000145 | Construct the flat Hermitian bundle explicitly as 000146 | \[ 000147 | L_F:=(\widetilde X_f^\circ\times\mathbb C^3)/\pi_1(X_f^\circ), 000148 | \] 000149 | where $\pi_1(X_f^\circ)$ acts on $\mathbb C^3$ through $\rho_F$. Because the image of $\rho_F$ lies 000150 | in $SU(3)_F$, the standard Hermitian form on $\mathbb C^3$ descends to a Hermitian metric on 000151 | $L_F$, and the trivial connection on $\widetilde X_f^\circ\times\mathbb C^3$ descends to a flat 000152 | Hermitian connection realizing the same monodromy representation. 000153 | 000154 | Conversely, any admissible flat Hermitian family connection with the same puncture data has the same 000155 | monodromy representation up to global $SU(3)_F$ conjugation. The unitary Riemann--Hilbert 000156 | correspondence for flat Hermitian bundles then identifies it with the descended bundle above. 000157 | Hence there is exactly one admissible flat Hermitian connection class realizing the rigid puncture 000158 | data. We denote this distinguished class by 000159 | \[ 000160 | [\nabla_F^\star]. 000161 | \] 000162 | \end{proof} 000163 |