Manuscript VII-D@1 · VII-D.tex · proposition · ef67c89c
Proposition: Exact positive-cutoff distribution and placement
The exact distribution and intersection coordinates › Positive-cutoff definition and regulator placement · lines 382–467 · proof included or linked
VII-D@1#prop:positive, VII-D@1#eq:Texact
The field regularization and the mixed-kernel convolution in (sc:placement) define the same insertion. Their numerical coefficient is
For every , this is a smooth function on , and
Its pairing on real product tests is exactly (sc:spectral).
Proof. and kernel convolution. For , transposition of convolution gives
Since is even, this is the kernel convolution displayed in (sc:placement). The identity holds on arbitrary smooth configurations: the original mixed kernel has compact support, and the convolution kernels are compactly supported.
-wave multiplier identities. The coefficients of are constant, so
for every smooth . For any constant tensor ,
This applies in particular to the de Donder polarizations in (sc:covariance). Applying the fixed operator to this equality retains the scalar multiplier . This proves the displayed formula for , without commuting through .
For the scalar leg, Euclidean radiality gives
The two scalar insertion slots therefore supply . The derivative factors are
multiplying the scalar spectral density gives (eq:Deps). The two insertion signs also multiply to . The middle observable is untouched.
and the product-test identity. For fixed positive , every coordinate derivative of the momentum integrands in and is integrable, locally uniformly in the observations. At zero momentum the only graviton denominators are and , locally integrable in three dimensions. The scalar density is locally integrable also for . At infinity the profiles provide arbitrary polynomial decay.
Thus (eq:Texact) is a product of smooth functions. Its compact-test bound follows by a supremum on a compact neighborhood of . Integrating against and using (eq:Deps) yields (sc:spectral).
Displayed formulas in this passage
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