The Riesz transform for homogeneous Schrödinger operators on metric cones

We consider Schroedinger operators on metric cones whose cross section is a closed Riemannian manifold $(Y, h)$ of dimension $d-1 \geq 2$. Thus the metric on the cone $M = (0, \infty)_r \times Y$ is $dr^2 + r^2 h$. Let $Δ$ be the Friedrichs Laplacian on $M$ and $V_0$ be a smooth function on $Y$, such that $Δ_Y + V_0 + (d-2)^2/4$ is a strictly positive operator on $L^2(Y)$, with lowest eigenvalue $μ^2_0$ and second lowest eigenvalue $μ^2_1$, with $μ_0, μ_1 > 0$. The operator we consider is $H = Δ+ V_0/r^2$, a Schrödinger operator with inverse square potential on $M$; notice that $H$ is homogeneous of degree -2. We study the Riesz transform $T = \nabla H^{-1/2}$ and determine the precise range of $p$ for which $T$ is bounded on $L^p(M)$. This is achieved by making a precise analysis of the operator $(H + 1)^{-1}$ and determining the complete asymptotics of its integral kernel. We prove that if $V$ is not identically zero, then the range of $p$ for $L^p$ boundedness is $d/ \Big(min(1+d/2+μ_0, d \Big) < p < d / \Big(max(d/2-μ_0, 0) \Big),$ while if $V$ is identically zero, then the range is $1 < p < d / \Big(max(d/2-μ_1, 0 \Big).$ The result in the case $V$ identically zero was first obtained in a paper by H.-Q. Li.

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