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2001 | OriginalPaper | Chapter

Brownian Motion on the Martin Space

Author : Joseph L. Doob

Published in: Classical Potential Theory and Its Probabilistic Counterpart

Publisher: Springer Berlin Heidelberg

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Let D be a connected Greenian subset of ℝN, let K be a Martin function for D, let h be a strictly positive superbarmonic function on D, and let {wξh(·), ℱξh(·)} be an h-Brownian motion in D from ξ with lifetime Sξh. For A a subset of D let SξhA and LξhA, respectively, be the hitting and last hitting times of A by wξh(·). According to Theorem l.XII.10, if h is harmonic, the Martin boundary is h-resolutive and μ D h(ξ, dζ) = K(ζ, ξ)M h (dζ)/h(ξ), where M h is the Martin representing measure of h corresponding to K. According to Theorem II.2, the left limit wξh(Sξh−) exists almost surely and has distribution μ D h(ξ, ·) supported (Section l.XII.7) by the minimal Martin boundary ∂1mD. In particular, if ζ is a minimal Martin boundary point and if h = K(ζ, ·), then μ D h(·, {ζ}) = 1; so wξh(Sξh−) = ζ almost surely. With this choice of h we shall sometimes write wξζ(·), SξζA, LξζA, respectively, for wξh(·), SξhA, LξhA.

Metadata
Title
Brownian Motion on the Martin Space
Author
Joseph L. Doob
Copyright Year
2001
Publisher
Springer Berlin Heidelberg
DOI
https://doi.org/10.1007/978-3-642-56573-1_32