Manuscript X-I-ST@1 · X-I-ST.tex · section · 9745fd40
Completion Green operators and causal compatibility
Free normalization and the exact free field limit › Completion Green operators and causal compatibility · lines 535–587
X-I-ST@1#eq:Grb, X-I-ST@1#eq:causalblocks
Let and be the positive equation inverses of and on . Their existence and causal support are standard on this globally hyperbolic completion BGP.
The metric–auxiliary inverse is
The scalar action-Hessian inverse is .
For clarity about odd signs, place Grassmann variations on the left. The ghost Euler derivatives are
In this source-dual convention their inverse is
Changing the order or parity convention for the odd source dual changes printed inverse matrices. It does not license changing the action or the causal brackets.
Put . The causal brackets used here have blocks
\begin{array}{c|c@{\qquad}c|c}
AB&\Delta_{AB}&AB&\Delta_{AB}\\ \hline
rr&-4\mathsf P_{\mathrm{tr}}\delta_0&\phi\phi&-\delta_m\\
rb&K\delta_0&br&-2\mathsf C\mathsf P_{\mathrm{tr}}\delta_0\\
c\bar c&-\delta_0&\bar c c&\delta_0
\end{array}
\label{eq:causalblocks}and . Thus the scalar sign and the odd signs are not inferred from an unsigned array.
Displayed formulas in this passage
X-I-ST@1#eq:Grb · line 544
X-I-ST@1#eq:causalblocks · line 575
\begin{array}{c|c@{\qquad}c|c} AB&\Delta_{AB}&AB&\Delta_{AB}\\ \hline rr&-4\mathsf P_{\mathrm{tr}}\delta_0&\phi\phi&-\delta_m\\ rb&K\delta_0&br&-2\mathsf C\mathsf P_{\mathrm{tr}}\delta_0\\ c\bar c&-\delta_0&\bar c c&\delta_0 \end{array} \label{eq:causalblocks}unlabeled · line 559
unlabeled · line 563