Conditional Gambler’s Ruin Problem with Arbitrary Winning and Losing Probabilities with Applications
In this paper we provide formulas for the expectation of a conditional game duration in a finite state-space one-dimensional gambler’s ruin problem with arbitrary winning p ( n ) and losing q ( n ) probabilities ( i.e., they depend on the current fortune). The formulas are stated in terms of the pa...
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Published in | Methodology and computing in applied probability Vol. 27; no. 3; p. 54 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
New York
Springer US
01.09.2025
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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Summary: | In this paper we provide formulas for the expectation of a conditional game duration in a finite state-space one-dimensional gambler’s ruin problem with arbitrary winning
p
(
n
) and losing
q
(
n
) probabilities (
i.e.,
they depend on the current fortune). The formulas are stated in terms of the parameters of the system. Beyer and Waterman (
Math Mag
,
50
(1):42–45, 1977) showed that for the classical gambler’s ruin problem the distribution of a conditional absorption time is symmetric in
p
and
q
. Our formulas imply that for non-constant winning/losing probabilities the expectation of a conditional game duration is symmetric in these probabilities (
i.e.,
it is the same if we exchange
p
(
n
) with
q
(
n
)) as long as a ratio
q
(
n
)/
p
(
n
) is constant. Most of the formulas are applied to a non-symmetric random walk on a circle/polygon. Moreover, for a symmetric random walk on a circle we construct an optimal strong stationary dual chain – which turns out to be an absorbing, non-symmetric, birth and death chain. We apply our results and provide a formula for its expected absorption time, which is the fastest strong stationary time for the aforementioned symmetric random walk on a circle. This way we improve upon a result of Diaconis and Fill (
Ann Prob
,
18
(4):1483–1522, 1990), where strong stationary time – however not the fastest – was constructed. Expectations of the fastest strong stationary time and the one constructed by Diaconis and Fill differ by 3/4, independently of a circle’s size. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
ISSN: | 1387-5841 1573-7713 |
DOI: | 10.1007/s11009-025-10181-7 |