2021
DOI: 10.1103/physrevresearch.3.013075
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First passage time distribution of active thermal particles in potentials

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Cited by 11 publications
(12 citation statements)
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“…with eigenvalue λ n = −n/L 2 , where H n (x) is the nth Hermite polynomial in the 'probabilists' convention', see appendix B [35,[42][43][44]. The functions u n (x) are similar to the so-called Hermite functions exp(−x 2 /(4L 2 )) H n (x/L).…”
Section: J Stat Mech (2021) 063203mentioning
confidence: 99%
“…with eigenvalue λ n = −n/L 2 , where H n (x) is the nth Hermite polynomial in the 'probabilists' convention', see appendix B [35,[42][43][44]. The functions u n (x) are similar to the so-called Hermite functions exp(−x 2 /(4L 2 )) H n (x/L).…”
Section: J Stat Mech (2021) 063203mentioning
confidence: 99%
“…The dimensionless parameter λ is the coupling strength and β is the return rate. The persistence time β −1 induces temporal correlations, or a memory, in the noise y(t) in a similar way to active fluctuations in the motion of active Ornstein-Uhlenbeck particles [33,34], Eq. (18).…”
Section: Branching Coupled To An Ornstein-uhlenbeck Processmentioning
confidence: 99%
“…In our recent work [26], we presented a scheme to calculate first-passage distributions for the same class of * bwalter@sissa.it non-Markovian processes. These results relied on a perturbative functional expansion of a renewal type equation inspired by the classical work of [10,27].…”
mentioning
confidence: 99%
“…Example: Brownian Motion driven by self-correlated noise-We briefly discuss the example process of active thermal Brownian motion (ATBM, [26]) on a real line. In our previous article [26], we found the perturbative correction to the first-passage time moment generating function for an active thermal Ornstein Uhlenbeck process, and an active Brownian Motion on a ring.…”
mentioning
confidence: 99%
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