If a tempered distribution u is smooth near a point x, then the pair (x, ω) is not in
the wavefront set of u for any direction ω.
The singular support of the Fourier transform of a compactly cut-off tempered distribution
φ · u is empty: the result is smooth everywhere.
If the conic singular support sphere of 𝓕(φ · u) is empty and φ is a smooth compactly
supported cutoff, then φ · u is itself a Schwartz function.
For any open set U and point x ∈ U, there exists a smooth compactly supported complex
bump function φ with φ x ≠ 0 and tsupport φ ⊆ U.
Converse to not_mem_wavefrontSet_of_isSmoothNear: if no direction (x, ω) belongs to the
wavefront set of u, then u is smooth near x. Uses compactness of the sphere of directions.
The projection to the base of the wavefront set is contained in the singular support.
The singular support is contained in the projection to the base of the wavefront set.
The projection to the base of the wavefront set equals the singular support.
The "boundary" subset of pairs (p, q) where at least one of the components corresponds to
a direction at infinity (an Sum.inr of Sphere n).
Instances For
The scattering wavefront set is always contained in the boundary subset boundaryOfProd.
The wavefront set of a tempered distribution is a closed subset of E n × Sphere n.
The singular support of a tempered distribution is closed in E n.
The cone singular support of a tempered distribution is closed in E n ⊕ Sphere n.
The set of sphere directions ω for which g is a conic cutoff near ω is open.
The scattering wavefront set at infinity is a closed subset of Sphere n × (E n ⊕ Sphere n).
The full scattering wavefront set (union of finite-part and at-infinity components) is closed.
If the first projection p is outside the cone singular support, then no pair (p, q)
belongs to the scattering wavefront set.
If g is a conic cutoff near ω, then the singular support of 𝓕(g · u) is empty: it is
smooth everywhere as the Fourier transform of a conically localized distribution.
A tempered distribution is itself given by a Schwartz function whenever its Fourier transform is.
If g is a conic cutoff near ω and the conic singular support sphere of 𝓕(g · u) is
empty, then g · u is given by a Schwartz function.
For any direction ω and open neighbourhood U of ω, there exists a function g that is
a conic cutoff near ω whose support is contained in U.
Converse direction for the cone singular support: if no second component q makes (p, q)
land in the scattering wavefront set, then p is outside the cone singular support.
The projection to the first factor of the scattering wavefront set is contained in the cone singular support.
The cone singular support is contained in the projection to the first factor of the scattering wavefront set.
The projection to the first factor of the scattering wavefront set equals the cone singular support.
Melrose Proposition 12.14: the scattering wavefront set lies in the boundary, both wavefront sets are closed, and the projections to the first factor recover the singular support and the cone singular support respectively.