Abstract
Abstract
We study the behaviour of a symmetric exclusion process in the presence of non-Markovian stochastic resetting, where the configuration of the system is reset to a step-like profile at power-law waiting times with an exponent α. We find that the power-law resetting leads to a rich behaviour for the currents, as well as density profile. We show that, for any finite system, for α < 1, the density profile eventually becomes uniform while for α > 1, an eventual non-trivial stationary profile is reached. We also find that, in the limit of thermodynamic system size, at late times, the average diffusive current grows
∼
t
θ
with
θ
=
1
/
2
for
α
⩽
1
/
2
,
θ
=
α
for
1
/
2
<
α
⩽
1
and θ = 1 for α > 1. We also analytically characterize the distribution of the diffusive current in the short-time regime using a trajectory-based perturbative approach. Using numerical simulations, we show that in the long-time regime, the diffusive current distribution follows a scaling form with an
α
−
dependent scaling function. We also characterise the behaviour of the total current using renewal approach. We find that the average total current also grows algebraically
∼
t
ϕ
where
ϕ
=
1
/
2
for
α
⩽
1
,
ϕ
=
3
/
2
−
α
for
1
<
α
⩽
3
/
2
, while for
α
>
3
/
2
the average total current reaches a stationary value, which we compute exactly. The standard deviation of the total current also shows an algebraic growth with an exponent
Δ
=
1
2
for
α
⩽
1
, and
Δ
=
1
−
α
2
for
1
<
α
⩽
2
, whereas it approaches a constant value for α > 2. The total current distribution remains non-stationary for α < 1, while, for α > 1, it reaches a non-trivial and strongly non-Gaussian stationary distribution, which we also compute using the renewal approach.
Subject
Statistics, Probability and Uncertainty,Statistics and Probability,Statistical and Nonlinear Physics
Cited by
5 articles.
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