SciPost Submission Page
Stochastic Resetting and Large Deviations
by Martin Evans, John Sunil
This is not the latest submitted version.
Submission summary
| Authors (as registered SciPost users): | Martin Evans |
| Submission information | |
|---|---|
| Preprint Link: | scipost_202412_00040v1 (pdf) |
| Date submitted: | Dec. 20, 2024, 8:56 p.m. |
| Submitted by: | Martin Evans |
| Submitted to: | SciPost Physics Lecture Notes |
| for consideration in Collection: |
| Ontological classification | |
|---|---|
| Academic field: | Physics |
| Specialties: |
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| Approach: | Theoretical |
Abstract
Stochastic resetting has been a subject of considerable interest within statistical physics, both as means of improving completion times of complex processes such as searches and as a paradigm for generating nonequilibrium stationary states. In these lecture notes we give a self-contained introduction to the toy model of diffusion with stochastic resetting. We also discuss large deviation properties of additive functionals of the process such as the cost of resetting. Finally, we consider the generalisation from Poissonian resetting, where the resetting process occurs with a constant rate, to non-Poissonian resetting.
Current status:
Reports on this Submission
Report #3 by Anonymous (Referee 2) on 2025-2-26 (Invited Report)
- Cite as: Anonymous, Report on arXiv:scipost_202412_00040v1, delivered 2025-02-26, doi: 10.21468/SciPost.Report.10728
Strengths
Weaknesses
Report
Requested changes
I found a few typos/errors in these notes, which the authors should correct.
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The factor $\sqrt{s}$ in the prefactor of the expression in equation (13) should be in the numerator, i.e., equation (13) should read $\widetilde{P}(x,s|x_0)=\frac{1}{2}\, \sqrt{\frac{s}{D}}\, e^{-\sqrt{\frac{s}{D}}\, |x-x_0| }$
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In line 143, "using" should be "Using"
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With the scaling variable $z=x_0/\sqrt{4 D t}$, equation (21) should read $-2z\frac{dg}{dz} = \frac{d^2 g}{dz^2}$. If the authors want to keep equation (21) unchanged, the correct scaling variable should be $z=x_0/\sqrt{D t}$.
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The sentence after equation (55) ends with a mathematical expression, and the following sentence again starts with a mathematical variable $y$. It might be better to rephrase the first part of the sentence. For example, "The dimensionless parameter $y$ is the ratio..."
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In line 289, expression (ii), both $s_0$ and $s$ appear. Is there a typo? Otherwise, give details.
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In equation (77) and line 370, perhaps $x_i$ in the argument of the theta function should be replaced by $x$.
Recommendation
Publish (surpasses expectations and criteria for this Journal; among top 10%)
Report #2 by Anonymous (Referee 2) on 2025-2-26 (Invited Report)
- Cite as: Anonymous, Report on arXiv:scipost_202412_00040v1, delivered 2025-02-26, doi: 10.21468/SciPost.Report.10727
Strengths
Weaknesses
Report
Requested changes
I found a few typos/errors in these notes, which the authors should correct.
-
The factor $\sqrt{s}$ in the prefactor of the expression in equation (13) should be in the numerator, i.e., equation (13) should read $\widetilde{P}(x,s|x_0)=\frac{1}{2}\, \sqrt{\frac{s}{D}}\, e^{-\sqrt{\frac{s}{D}}\, |x-x_0| }$
-
In line 143, "using" should be "Using"
-
With the scaling variable $z=x_0/\sqrt{4 D t}$, equation (21) should read $-2z\frac{dg}{dz} = \frac{d^2 g}{dz^2}$. If the authors want to keep equation (21) unchanged, the correct scaling variable should be $z=x_0/\sqrt{D t}$.
-
The sentence after equation (55) ends with a mathematical expression, and the following sentence again starts with a mathematical variable $y$. It might be better to rephrase the first part of the sentence. For example, "The dimensionless parameter $y$ is the ratio..."
-
In line 289, expression (ii), both $s_0$ and $s$ appear. Is there a typo? Otherwise, give details.
-
In equation (77) and line 370, perhaps $x_i$ in the argument of the theta function should be replaced by $x$.
Recommendation
Publish (surpasses expectations and criteria for this Journal; among top 10%)
Report #1 by Anonymous (Referee 1) on 2025-2-13 (Invited Report)
- Cite as: Anonymous, Report on arXiv:scipost_202412_00040v1, delivered 2025-02-13, doi: 10.21468/SciPost.Report.10664
Report
The present manuscript represents an interesting lecture notes on stochastic resetting and the large deviation in stochastic resetting, which is of interest to analyze the transition to the nonequilibrium stationary state of the system in the long time limit. It also deals with the cost of resetting. The topic of stochastic resetting has been considered as a hot topic in nonequilibrium statistical physics in the last decade and it is still a mechanism which is used to explain different phenomena, for example, in economy. Therefore, the manuscript is appropriate for publication in SciPost Physics Lecture Notes.
Here are some additional comment to the manuscript.
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It would be nice if Authors mention that the nonequilibrium stationary state (34) is the Laplace distribution. Graphical representation of it would be useful, from where the cusp at the origin could be visible.
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It could be useful if the Authors give the renewal equation in Laplace domain, fro $x_0=x_r$, which will yield
$$\tilde{P}_r(x,s|x_r)=\frac{s+r}{s} P_0(x,s+r|x_r),$$from where one can easily find the nonequilibrium stationary state reached in the long time limit, which is actually eq. (40),$$P^{\ast}(x)=r\hat{P}_0(x,r|x_r),$$by using the final value theorem of the Laplace transform,$$\lim_{t→\infty}f(t) = \lim_{s→0}s\hat{f}(s).$$ -
Graphical representation of the MFPT vs resetting rate could be useful in order to see that there is an optimal resetting rate which minimizes the MFPT.
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When talking about general resetting distribution, useful reference could be [Phys. Rev. E 99, 012141 (2019)].
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Optional, it could be useful if the Authors show the transition of the mean squared displacement from normal diffusion in the short time limit to saturation in the long time limit due to the resetting of the particle.
Recommendation
Publish (surpasses expectations and criteria for this Journal; among top 10%)
