Abstract
Recently the authors showed that the Martin boundary and the minimal Martin boundary for a censored (or resurrected) α-stable process Y in a bounded C1,1-open set D with α ∈ (1, 2) can all be identified with the Euclidean boundary ∂ D of D. Under the gaugeability assumption, we show that the Martin boundary and the minimal Martin boundary for the Schrödinger operator obtained from Y through a non-local Feynman-Kac transform can all be identified with ∂ D. In other words, the Martin boundary and the minimal Martin boundary are stable under non-local Feynman-Kac perturbations. Moreover, an integral representation of nonnegative excessive functions for the Schrödinger operator is explicitly given. These results in fact hold for a large class of strong Markov processes, as are illustrated in the last section cf this paper. As an application, the Martin boundary for censored relativistic stable processes in bounded C1,1-smooth open sets is studied in detail.
| Original language | English |
|---|---|
| Pages (from-to) | 525-564 |
| Number of pages | 40 |
| Journal | Probability Theory and Related Fields |
| Volume | 128 |
| Issue number | 4 |
| DOIs | |
| Publication status | Published - Apr 2004 |
| Externally published | Yes |
Keywords
- Excessive function
- Feynman-Kac transform
- Green function
- Martin boundary
- Martin integral representation
- Martin kernel
- Minimal harmonic function
- Non-local perturbation
- Resurrection
- Schrödinger semigroup
- Stable process
- h-transform