TFPT scientific source excerpt Original repository path: documents/archive--paper-latex--tfpt-42/sections/007-subsection-carrier-form-of-the-electromagnetic-closure.tex Original file SHA-256: 6f98cfb7404f415e4a511712c1fa144c85bb662c36386cc32d1ebb3537a9fb6b Inclusive original lines: 13-77 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. 000013 | \begin{proposition}[Carrier susceptibility exponent] 000014 | \label{prop:carrier-susceptibility-exponent} 000015 | On the minimal carrier branch, 000016 | \[ 000017 | B\gamma=\frac32\cdot\frac56=\frac54. 000018 | \] 000019 | \end{proposition} 000020 | \begin{definition}[Minimal primitive seam transfer] 000021 | \label{def:exact-seam-generating-function} 000022 | Let $\psi_{\Sigma}$ be the normalized primitive seam mode singled out by 000023 | \Cref{thm:primitive-seam-generator}. Define the minimal seam transfer operator by the rank-one 000024 | projector 000025 | \[ 000026 | U_{\Sigma}^{\min}:=|\psi_{\Sigma}\rangle\langle\psi_{\Sigma}|. 000027 | \] 000028 | With 000029 | \[ 000030 | q(\alpha):=\deltatop e^{-2\alpha}, 000031 | \qquad 000032 | B\gamma=\frac54, 000033 | \] 000034 | one has 000035 | \[ 000036 | \mathcal W_{\Sigma}(\alpha) 000037 | := 000038 | -B\gamma\,\tr_{\mathrm{adm}}\log\!\bigl(1-q(\alpha)U_{\Sigma}^{\min}\bigr) 000039 | =-\frac54\log(1-q(\alpha)). 000040 | \] 000041 | \[ 000042 | \mathcal T_{\Sigma}(\alpha)=e^{\mathcal W_{\Sigma}(\alpha)}=(1-q(\alpha))^{-5/4}. 000043 | \] 000044 | \begin{equation} 000045 | \label{eq:phi-opening} 000046 | \phiseam(\alpha)=\phibase+q(\alpha)(1-q(\alpha))^{-5/4}. 000047 | \end{equation} 000048 | \end{definition} 000049 | 000050 | \begin{proposition}[Normalized scalar closure potential] 000051 | \label{prop:log-det-variation-u1} 000052 | Let 000053 | \[ 000054 | F_{U(1)}(\alpha):=\alpha^3-2\cthree^3\alpha^2-8\cthree^6 b_1\log\bigl(\phiseam(\alpha)^{-1}\bigr). 000055 | \] 000056 | There exists a unique quartic local counterterm $P_{\mathrm{loc}}$ satisfying 000057 | \[ 000058 | P_{\mathrm{loc}}(0)=P_{\mathrm{loc}}'(0)=0, 000059 | \qquad 000060 | P_{\mathrm{loc}}'(\alpha)=\alpha^3-2\cthree^3\alpha^2, 000061 | \] 000062 | namely 000063 | \[ 000064 | P_{\mathrm{loc}}(\alpha)=\frac{\alpha^4}{4}-\frac23\cthree^3\alpha^3. 000065 | \] 000066 | Hence the normalized scalar closure potential 000067 | \[ 000068 | \Gamma_{U(1)}(\alpha) 000069 | := 000070 | \frac{\alpha^4}{4}-\frac23\cthree^3\alpha^3 000071 | -8\cthree^6 b_1\int_0^\alpha \log\bigl(\phiseam(a)^{-1}\bigr)\,da 000072 | \] 000073 | satisfies 000074 | \[ 000075 | \partial_{\alpha}\Gamma_{U(1)}(\alpha)=F_{U(1)}(\alpha). 000076 | \] 000077 | \end{proposition}