Manuscript XI-B@1 · XI-B.tex · proposition · 063b989e
Proposition: Full auxiliary inverse
Causal Green operators and their normalization › The independent auxiliary block · lines 712–753 · proof included or linked
XI-B@1#prop:aux, XI-B@1#eq:Gaux
The unique retarded and advanced inverses are
G^{\mathrm{aux}}^\pm=
\begin{pmatrix}
G^{\mathrm{gr}}^\pm&G^{\mathrm{gr}}^\pm D^*\\
DG^{\mathrm{gr}}^\pm&DG^{\mathrm{gr}}^\pm D^*-\frac12\operatorname{id}
\end{pmatrix}
=
\begin{pmatrix}
-\mathcal P\mathsf E_0^\pm&\mathcal R\mathsf E_0^\pm\\
D(-\mathcal P\mathsf E_0^\pm)&0
\end{pmatrix}.
\label{eq:Gaux}The identities in the second matrix hold on compact interior sources.
Proof. The auxiliary equation gives . Substitution reduces the metric equation to
The handed-off identity is . Equation (eq:Ggr) therefore gives the first matrix and uniqueness.
For the simplification, direct calculation gives
Consequently
and
DG^{\mathrm{gr}}^\pm D^*=\frac12\operatorname{id}.
The last block cancels the algebraic contact term.
The source elimination proves both Green identities; derivatives
do not enlarge causal support.
Displayed formulas in this passage
XI-B@1#eq:Gaux · line 715
G^{\mathrm{aux}}^\pm= \begin{pmatrix} G^{\mathrm{gr}}^\pm&G^{\mathrm{gr}}^\pm D^*\\ DG^{\mathrm{gr}}^\pm&DG^{\mathrm{gr}}^\pm D^*-\frac12\operatorname{id} \end{pmatrix} = \begin{pmatrix} -\mathcal P\mathsf E_0^\pm&\mathcal R\mathsf E_0^\pm\\ D(-\mathcal P\mathsf E_0^\pm)&0 \end{pmatrix}. \label{eq:Gaux}unlabeled · line 735
unlabeled · line 743