Manuscript X-F-ST@1 · X-F-ST.tex · section · e71f03ef

Derivation of the prescribed response equation

F2: background gauge, kinetic correction, and retarded jet law › Derivation of the prescribed response equation · lines 947–999

X-F-ST@1#eq:fluctuation, X-F-ST@1#eq:response

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Consider formally

Its fluctuation Euler derivative through first order is

This follows directly from Lemma lem:action, polarization, and (eq:backgroundgauge).

The background-field prescription removes the terms independent of the fluctuation from its equation: equivalently, it removes constant and linear fluctuation terms from the local action expansion. It does not remove the linear kinetic equation. The classical backgrounds are not solved for.

Now write the fluctuation as , and multiply the order- gravitational sources, after Euler differentiation, by . The resulting definition is

For smooth inputs this is the unique zero-past solution of .

Every source in (eq:response) is past-compact: its intersection with the causal past of a compact set is compact. This follows from its vanishing for and flat finite propagation. No spatial decay is needed BGP. Without onset multiplication the self source of a general free field is not past-compact, and the retarded Green operator cannot be applied on that basis.

Displayed formulas in this passage

  • X-F-ST@1#eq:fluctuation · line 956

  • X-F-ST@1#eq:response · line 979

  • unlabeled · line 950