“…where ν is the Lévy intensity and A = σσ T is the diffusion matrix of (X t ) t≥0 , and where we use the notation σ∇ · σ∇f (x) = d i,j=1 (σσ T ) ij ∂ x i ∂ x j f (x). Under suitable conditions (see a discussion in [27]), the GST process satisfies a stochastic differential equation with jumps of the form where (B t ) t≥0 is standard Brownian motion, N is a Poisson random measure on [0, ∞) × R d × [0, ∞) with intensity dtν(z)dzdv, and N is the related compensated Poisson measure. From the above two observations it is seen that the potential V perturbing the Lévy process enters the GST process via the ground state ϕ 0 of the operator H, and in general gives rise to a position-dependent drift and a position-dependent bias in the jump kernel, i.e., a Lévy-type process.…”