The planar Newtonian kernel away from its pole #
This file introduces the logarithmic kernel for the negative Laplacian on the complex plane,
G(z) = -(2 * π)⁻¹ * log ‖z‖,
and establishes its classical pointwise properties away from the pole. In particular, G and
each translate z ↦ G (z - a) are harmonic away from their poles. The distributional identity
-Δ G = δ₀, which fixes the normalization by computing the flux through a circle, is deliberately
left to the later distributional development of the fundamental solution.
The harmonicity proof consumes Mathlib's AnalyticAt.harmonicAt_log_norm, applied to the identity
or to z ↦ z - a. The remaining results record the translation, symmetry, and scaling API used
when the kernel is integrated against a source to form a Newtonian potential.
Main declarations #
TauCeti.planarNewtonianKernel: the logarithmic kernel for-Δonℂ.TauCeti.harmonicAt_planarNewtonianKernel: harmonicity away from the origin.TauCeti.harmonicAt_planarNewtonianKernel_sub: harmonicity of a kernel with polea.TauCeti.laplacian_planarNewtonianKernel: the pointwise equationΔ G = 0off the pole.
The Newtonian kernel for the negative Laplacian on the plane, represented as ℂ.
The value assigned at the pole is immaterial for the pointwise theory in this file. Lean's
convention Real.log 0 = 0 makes this a total function; analytically, the kernel has a logarithmic
singularity there.
Instances For
The planar Newtonian kernel is invariant under multiplication by a unit complex number.
Scaling the argument adds the logarithm of the scale to the planar Newtonian kernel.
The kernel with pole a is symmetric in its two spatial arguments.
The translated kernel z ↦ G(z - a) is harmonic at every point other than its pole a.
The logarithmic Newtonian kernel is harmonic at every point away from its pole at 0.
The planar Newtonian kernel is harmonic on the punctured plane.
A planar Newtonian kernel with pole a is harmonic on the complement of that pole.
Away from its pole, a translated planar Newtonian kernel is twice continuously differentiable.
Away from its pole, the planar Newtonian kernel is twice continuously differentiable.
The planar Newtonian kernel solves the homogeneous Laplace equation pointwise away from its pole. Its nonzero distributional Laplacian is concentrated at the omitted pole.
A translated planar Newtonian kernel solves the homogeneous Laplace equation away from its pole.