A point p of the closed unit ball is "on the sphere" if its underlying
norm equals 1.
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The disjoint scattering wavefront set condition that ensures the product
u · v of two tempered distributions is well-defined: for every point p of
the closed unit ball and every direction ω on the sphere, if (p, ω) lies
in the scattering wavefront set of u, then the antipodal direction
(p, -ω) must not lie in the scattering wavefront set of v.
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The disjoint scattering wavefront set condition that ensures the
convolution u ∗ v of two tempered distributions is well-defined: for every
direction θ on the sphere and every point q of the closed unit ball, if
(θ, q) lies in the scattering wavefront set of u, then (-θ, q) must not
lie in the scattering wavefront set of v. This is the Fourier-dual of
DisjointWFscProductCondition.
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Construction of the convolution u ∗ v of two tempered distributions
under the disjoint scattering wavefront set condition for convolution.
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The convolution constructed via a Schwartz / compactly-supported
decomposition of the pair (u, v) does not depend on the choice of
decomposition. This is the well-definedness statement underlying
Lemma 12.6 of Melrose.
The disjoint scattering wavefront set condition for products of u and
v translates, via the Fourier transform, into the disjoint scattering
wavefront set condition for convolutions of 𝓕 u and 𝓕 v. This is the
Fourier exchange between products and convolutions of distributions
(Theorem 12.18 of Melrose).
Construction of the product u · v of two tempered distributions under
the disjoint scattering wavefront set condition for products. The product is
defined by reducing to the convolution of 𝓕 u and 𝓕 v via the Fourier
transform.
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Packaged form of the well-definedness statement of Theorem 12.18 of Melrose: under the appropriate disjoint scattering wavefront set conditions, the product and convolution of two tempered distributions are simultaneously well-defined.