TFPT scientific source excerpt Original repository path: documents/archive--tfpt-45--source_extracts--03_em_flavor_source/sections/001-section-kernel-numerics-and-electromagnetic-closure.tex Original file SHA-256: 5fdbdc1b7d8af7f85e5fc2435f567402b3dbcb96938951e58e633cf42549c7e2 Inclusive original lines: 95-150 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. 000095 | \label{def:exact-seam-generating-function} 000096 | Let $\psi_{\Sigma}$ be the normalized primitive seam mode singled out by 000097 | \TFPTxref{thm:primitive-seam-generator}. Define the minimal seam transfer operator by the rank-one 000098 | projector 000099 | \[ 000100 | U_{\Sigma}^{\min}:=|\psi_{\Sigma}\rangle\langle\psi_{\Sigma}|. 000101 | \] 000102 | With 000103 | \[ 000104 | q(\alpha):=\deltatop e^{-2\alpha}, 000105 | \qquad 000106 | B\gamma=\frac54, 000107 | \] 000108 | one has 000109 | \[ 000110 | \mathcal W_{\Sigma}(\alpha) 000111 | := 000112 | -B\gamma\,\tr_{\mathrm{adm}}\log\!\bigl(1-q(\alpha)U_{\Sigma}^{\min}\bigr) 000113 | =-\frac54\log(1-q(\alpha)). 000114 | \] 000115 | \[ 000116 | \mathcal T_{\Sigma}(\alpha)=e^{\mathcal W_{\Sigma}(\alpha)}=(1-q(\alpha))^{-5/4}. 000117 | \] 000118 | \begin{equation} 000119 | \label{eq:phi-opening} 000120 | \phiseam(\alpha)=\phibase+q(\alpha)(1-q(\alpha))^{-5/4}. 000121 | \end{equation} 000122 | \end{definition} 000123 | 000124 | \begin{proposition}[Normalized scalar closure potential] 000125 | \label{prop:log-det-variation-u1} 000126 | Let 000127 | \[ 000128 | F_{U(1)}(\alpha):=\alpha^3-2\cthree^3\alpha^2-8\cthree^6 b_1\log\bigl(\phiseam(\alpha)^{-1}\bigr). 000129 | \] 000130 | There exists a unique quartic local counterterm $P_{\mathrm{loc}}$ satisfying 000131 | \[ 000132 | P_{\mathrm{loc}}(0)=P_{\mathrm{loc}}'(0)=0, 000133 | \qquad 000134 | P_{\mathrm{loc}}'(\alpha)=\alpha^3-2\cthree^3\alpha^2, 000135 | \] 000136 | namely 000137 | \[ 000138 | P_{\mathrm{loc}}(\alpha)=\frac{\alpha^4}{4}-\frac23\cthree^3\alpha^3. 000139 | \] 000140 | Hence the normalized scalar closure potential 000141 | \[ 000142 | \Gamma_{U(1)}(\alpha) 000143 | := 000144 | \frac{\alpha^4}{4}-\frac23\cthree^3\alpha^3 000145 | -8\cthree^6 b_1\int_0^\alpha \log\bigl(\phiseam(a)^{-1}\bigr)\,da 000146 | \] 000147 | satisfies 000148 | \[ 000149 | \partial_{\alpha}\Gamma_{U(1)}(\alpha)=F_{U(1)}(\alpha). 000150 | \]