Abstract
The classic Poisson formula giving an integral representation of bounded harmonic functions in the unit disk in terms of its boundary values has a long history (as it follows from its very name). Given a Markov operator P on a state space X one can easily define harmonic functions as invariant functions of the operator P, but in order to speak about their boundary values one needs a boundary, because no boundary is normally attached to the state space of a Markov chain (as distinct from bounded Euclidean domains common for the classic potential theory).
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Kaimanovich, V.A. (1992). Measure-Theoretic Boundaries of Markov Chains, 0–2 Laws and Entropy. In: Picardello, M.A. (eds) Harmonic Analysis and Discrete Potential Theory. Springer, Boston, MA. https://doi.org/10.1007/978-1-4899-2323-3_13
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DOI: https://doi.org/10.1007/978-1-4899-2323-3_13
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