The heat kernel gradient against a fixed test field #
For a smooth compactly supported test field ψ, the pairing
K_ij(y, r) = ∫ ψ_i(x) ∂_jΓ(x - y, r) dx is, after an integration by parts,
minus the heat semigroup applied to ∂_jψ_i. It is therefore bounded by a
multiple of (1 + |y|)^{-3} uniformly in r, continuous in r ≠ 0, and
vanishes for r ≤ 0. Without the integration by parts, the absolute pairing
is bounded by r^{-1/2} (1 + |y|)^{-3}. These are the kernel estimates behind
the time continuity of the forced heat response in prop:pv-local-solution.
The heat semigroup applied to |φ|, for a continuous compactly supported
φ, decays like (1 + |y|)^{-3} uniformly in time.
Each spatial derivative of the heat kernel is bounded by r^{-1/2} times the
heat kernel at the doubled time.
The pairing K_ij(y, r) = ∫ ψ_i(x) ∂_jΓ(x - y, r) dx of the spatial
derivative of the heat kernel, centred at y, with a component of a test
field.
Equations
- ESS.testKernelPairing ψ i j y r = ∫ (x : CKN.Foundation.Parabolic.Vec3), ψ x i * CKN.Foundation.Heat.heatKernelSpaceDerivative (x - y) r j
Instances For
The test pairing vanishes at nonpositive times.
The test pairing is jointly measurable in the centre and the time.
Integration by parts: at positive times the test pairing is minus the heat
semigroup applied to ∂_jψ_i.
The test pairing is bounded by a multiple of (1 + |y|)^{-3}, uniformly in time.
The test pairing is continuous in time away from r = 0.
Without integration by parts, the absolute test pairing is bounded by
r^{-1/2} (1 + |y|)^{-3}.