@article{
 title = {Quantifying a resonant-activation-like phenomenon in non-Markovian systems},
 type = {article},
 year = {2014},
 volume = {89},
 id = {fd411413-029a-3a8f-a143-de6a4656a300},
 created = {2020-10-30T10:12:15.580Z},
 file_attached = {false},
 profile_id = {f5390430-7317-381a-8c56-e25a878d78ef},
 last_modified = {2020-10-30T10:12:15.580Z},
 read = {false},
 starred = {false},
 authored = {true},
 confirmed = {false},
 hidden = {false},
 private_publication = {false},
 abstract = {Resonant activation is an effect of a noise-induced escape over a modulated potential barrier. The modulation of an energy landscape facilitates the escape kinetics and makes it optimal as measured by the mean first-passage time. A canonical example of resonant activation is a Brownian particle moving in a time-dependent potential under action of Gaussian white noise. Resonant activation is observed not only in typical Markovian-Gaussian systems but also in far-from-equilibrium and far-from-Markovianity regimes. We demonstrate that using an alternative to the mean first-passage time, robust measures of resonant activation, the signature of this effect can be observed in general continuous-time random walks in modulated potentials, even in situations when the mean first-passage time diverges. © 2014 American Physical Society.},
 bibtype = {article},
 author = {Szczepaniec, K. and Dybiec, B.},
 doi = {10.1103/PhysRevE.89.042138},
 journal = {Physical Review E - Statistical, Nonlinear, and Soft Matter Physics},
 number = {4}
}

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