Linear growth of the pressure potentials #
Combining the far-field decay of Newtonian potentials of compactly supported
data with the ball estimate for the radial weight ‖x‖ ^ (-3/2) gives, for each
of the three potential shapes N * g, ∂ⱼN * g and ∂ᵢ∂ⱼN * g, exactly the
pair of hypotheses consumed by the Liouville theorem
CKN.Foundation.Heat.weaklyHarmonicOn_eq_zero_of_lpNorm_linear_growth: local
L^{3/2} membership on every round ball about the origin, and a growth bound of
the form C * (1 + ρ). This is the decay-at-infinity input to the uniqueness
half of the Newtonian representation ext:newtonian of the paper.
The local L^{3/2} hypothesis near the origin is left to the consumer: for the
zeroth-order potential it follows from local integrability of the kernel, and for
the derivative potentials it is the Calderón–Zygmund bound.
The first-derivative Newtonian potential of integrable data supported in the
closed ball of radius R about x₀ satisfies the Liouville growth hypotheses.