Manuscript XII-C@1 · XII-C.tex · section · dead1004

C4: successor data without a response

C4: successor data without a response · lines 1229–1243

The action supplies a local quadratic source and its polarized form

J_{3, D} (γ_{1}, γ_{2}) = \frac{1}{2} [J_{3, D} [γ_{1} + γ_{2}] - J_{3, D} [γ_{1}] - J_{3, D} [γ_{2}]] .

This definition applies equally to the displayed layer terms. It contains no propagator.

Displayed formulas in this passage

unlabeled · line 1234
$J_{3, D} (γ_{1}, γ_{2}) = \frac{1}{2} [J_{3, D} [γ_{1} + γ_{2}] - J_{3, D} [γ_{1}] - J_{3, D} [γ_{2}]] .$