TFPT scientific source excerpt Original repository path: documents/archive--paper-latex--tfpt-42/sections/012-subsection-bosonic-relative-index-and-higgs-selection.tex Original file SHA-256: 8140f7618b51292b8acf79fdc999cac9482842626ed07db4edb54dc91c9499d6 Inclusive original lines: 3-82 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. 000003 | \begin{theorem}[Minimal determinant classes from the primitive charge generator] 000004 | \label{thm:determinant-class-higgs-selection} 000005 | \label{thm:determinant-clutching} 000006 | Let 000007 | \[ 000008 | L_2:=\det E_2, 000009 | \qquad 000010 | L_3:=\det E_3 000011 | \] 000012 | over the compactified oriented normal sphere $S^2=D_N\cup_{S^1}D_S$. Then the primitive charge 000013 | generator 000014 | \[ 000015 | X=-2P_3+3P_2 000016 | \] 000017 | together with center neutrality and seam-evenness forces the clutching map 000018 | \[ 000019 | g_2(\varphi)=e^{i\varphi} 000020 | \] 000021 | for $L_2$, while center neutrality forces 000022 | \[ 000023 | g_3(\varphi)=1 000024 | \] 000025 | for $L_3$. Therefore 000026 | \[ 000027 | c_1(L_2)=\deg g_2=1, 000028 | \qquad 000029 | c_1(L_3)=\deg g_3=0. 000030 | \] 000031 | This pair is the unique minimal nonnegative admissible determinant class. 000032 | \end{theorem} 000033 | 000034 | \begin{proof} 000035 | Complex line bundles on 000036 | \[ 000037 | S^2=D_N\cup_{S^1}D_S 000038 | \] 000039 | are classified by their clutching maps along the equator: 000040 | \[ 000041 | \pi_1(U(1))\cong \mathbb Z. 000042 | \] 000043 | Hence the first Chern class is exactly the winding degree of the transition function. 000044 | 000045 | In the weak rank-two sector the primitive charge generator 000046 | \[ 000047 | X=-2P_3+3P_2 000048 | \] 000049 | assigns the unique positive determinant winding to the seam-even weak block. The spin lift on the 000050 | oriented normal sphere acts there by the half-angle representation, so on the determinant line the 000051 | transition factor is 000052 | \[ 000053 | g_2(\varphi)=e^{i\varphi}, 000054 | \] 000055 | hence 000056 | \[ 000057 | \deg g_2=1, 000058 | \qquad 000059 | c_1(L_2)=1. 000060 | \] 000061 | 000062 | In the color sector admissibility imposes center neutrality. Therefore the determinant transition 000063 | function of the color block is null-homotopic and may be chosen constant: 000064 | \[ 000065 | g_3(\varphi)=1. 000066 | \] 000067 | Consequently 000068 | \[ 000069 | \deg g_3=0, 000070 | \qquad 000071 | c_1(L_3)=0. 000072 | \] 000073 | 000074 | The full primitive seam twist is therefore exhausted in the weak determinant class. Any nonnegative 000075 | pair strictly smaller than $(1,0)$ would force vanishing weak determinant winding and hence remove 000076 | the seam-even weak line required by the primitive charge generator. Any larger nonnegative pair 000077 | would insert extra clutching not carried by the primitive generator and therefore violate 000078 | minimality. Thus the unique minimal nonnegative admissible determinant class is 000079 | \[ 000080 | (c_1(L_2),c_1(L_3))=(1,0). 000081 | \] 000082 | \end{proof}