TFPT scientific source excerpt Original repository path: documents/archive--tfpt-45--source_extracts--04_qft_source/sections/005-subsection-admissible-schwinger-functions-minkowski-loca.tex Original file SHA-256: 8bf0a37157505ca12b90154dbe41a29c49a503686a8493dffd63945f205e0af6 Inclusive original lines: 144-160 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. 000144 | \begin{definition}[Admissible Schwinger functions] 000145 | \label{def:admissible-schwinger-functions} 000146 | Let 000147 | \[ 000148 | W_{\mathrm{rel}}[J,\eta,\bar\eta]:=\log Z_{\mathrm{rel}}[J,\eta,\bar\eta]. 000149 | \] 000150 | For local source insertions supported in the Euclidean continuation of 000151 | $\mathcal U_{\mathrm{scat}}$, define the truncated admissible Schwinger distributions by 000152 | \[ 000153 | S_n^T(x_1,\ldots,x_n) 000154 | := 000155 | \left. 000156 | \frac{\delta^n W_{\mathrm{rel}}}{\delta\mathcal J(x_1)\cdots\delta\mathcal J(x_n)} 000157 | \right|_{\mathcal J=0}, 000158 | \qquad 000159 | \mathcal J:=(J,\eta,\bar\eta). 000160 | \]