Extremal statistics for first-passage trajectories of drifted Brownian motion under stochastic resetting
We study the extreme value statistics of first-passage trajectories generated from a one-dimensional drifted Brownian motion subject to stochastic resetting to the starting point with a constant rate r . Each stochastic trajectory starts from a positive position x 0 and terminates whenever the parti...
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Veröffentlicht in: | Journal of statistical mechanics 2024-02, Vol.2024 (2), p.23209 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | We study the extreme value statistics of first-passage trajectories generated from a one-dimensional drifted Brownian motion subject to stochastic resetting to the starting point with a constant rate
r
. Each stochastic trajectory starts from a positive position
x
0
and terminates whenever the particle hits the origin for the first time. We obtain an exact expression for the marginal distribution
P
r
(
M
|
x
0
)
of the maximum displacement
M
. We find that stochastic resetting has a profound impact on
P
r
(
M
|
x
0
)
and the expected value
⟨
M
⟩
of
M
. Depending on the drift velocity
v
,
⟨
M
⟩
shows three distinct trends of change with
r
. For
v
⩾
0
,
⟨
M
⟩
decreases monotonically with
r
, and tends to
2
x
0
as
r
→
∞
. For
v
c
<
v
<
0
,
⟨
M
⟩
shows a nonmonotonic dependence on
r
, in which a minimum
⟨
M
⟩
exists for an intermediate level of
r
. For
v
⩽
v
c
,
⟨
M
⟩
increases monotonically with
r
. Moreover, by deriving the propagator and using a path decomposition technique, we obtain, in the Laplace domain, the joint distribution of
M
and the time
t
m
at which the maximum
M
is reached. Interestingly, the dependence of the expected value
⟨
t
m
⟩
of
t
m
on
r
is either monotonic or nonmonotonic, depending on the value of
v
. For
v
>
v
m
, there is a nonzero resetting rate at which
⟨
t
m
⟩
attains its minimum. Otherwise,
⟨
t
m
⟩
increases monotonically with
r
. We provide an analytical determination of two critical values of
v
,
v
c
≈
−
1.694
15
D
/
x
0
and
v
m
≈
−
1.661
02
D
/
x
0
, where
D
is the diffusion constant. Finally, numerical simulations are performed to support our theoretical results. |
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ISSN: | 1742-5468 1742-5468 |
DOI: | 10.1088/1742-5468/ad2678 |