TY - JOUR
T1 - Exact first-passage time distributions for three random diffusivity models
AU - Grebenkov, Denis S.
AU - Sposini, Vittoria
AU - Metzler, Ralf
AU - Oshanin, Gleb
AU - Seno, Flavio
N1 - Publisher Copyright:
© 2021 IOP Publishing Ltd
PY - 2021/1/29
Y1 - 2021/1/29
N2 - We study the extremal properties of a stochastic process xt defined by a Langevin equation x t = √2D0V(Bt) ξt, where ξt is a Gaussian white noise with zero mean, D0 is a constant scale factor, and V(Bt) is a stochastic 'diffusivity' (noise strength), which itself is a functional of independent Brownian motion Bt. We derive exact, compact expressions in one and three dimensions for the probability density functions (PDFs) of the first passage time (FPT) t from a fixed location x0 to the origin for three different realisations of the stochastic diffusivity: a cut-off case V(Bt) = Θ(Bt) (model I), where Θ(z) is the Heaviside theta function; a geometric Brownian motion V(Bt) = exp(Bt) (model II); and a case with V(Bt) = B2t (model III). We realise that, rather surprisingly, the FPT PDF has exactly the Lévy-Smirnov form (specific for standard Brownian motion) for model II, which concurrently exhibits a strongly anomalous diffusion. For models I and III either the left or right tails (or both) have a different functional dependence on time as compared to the Lévy-Smirnov density. In all cases, the PDFs are broad such that already the first moment does not exist. Similar results are obtained in three dimensions for the FPT PDF to an absorbing spherical target.
AB - We study the extremal properties of a stochastic process xt defined by a Langevin equation x t = √2D0V(Bt) ξt, where ξt is a Gaussian white noise with zero mean, D0 is a constant scale factor, and V(Bt) is a stochastic 'diffusivity' (noise strength), which itself is a functional of independent Brownian motion Bt. We derive exact, compact expressions in one and three dimensions for the probability density functions (PDFs) of the first passage time (FPT) t from a fixed location x0 to the origin for three different realisations of the stochastic diffusivity: a cut-off case V(Bt) = Θ(Bt) (model I), where Θ(z) is the Heaviside theta function; a geometric Brownian motion V(Bt) = exp(Bt) (model II); and a case with V(Bt) = B2t (model III). We realise that, rather surprisingly, the FPT PDF has exactly the Lévy-Smirnov form (specific for standard Brownian motion) for model II, which concurrently exhibits a strongly anomalous diffusion. For models I and III either the left or right tails (or both) have a different functional dependence on time as compared to the Lévy-Smirnov density. In all cases, the PDFs are broad such that already the first moment does not exist. Similar results are obtained in three dimensions for the FPT PDF to an absorbing spherical target.
KW - Diffusing diffusivity
KW - First-passage time
KW - Levy-Smirnow density
U2 - 10.1088/1751-8121/abd42c
DO - 10.1088/1751-8121/abd42c
M3 - Article
AN - SCOPUS:85099176849
SN - 1751-8113
VL - 54
JO - Journal of Physics A: Mathematical and Theoretical
JF - Journal of Physics A: Mathematical and Theoretical
IS - 4
M1 - 04LT01
ER -