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重置条件下的分数阶电报方程:非平衡稳态与首次通过时间

Fractional Telegrapher's Equation under Resetting: Non-Equilibrium Stationary States and First-Passage Times.

作者信息

Górska Katarzyna, Sevilla Francisco J, Chacón-Acosta Guillermo, Sandev Trifce

机构信息

Institute of Nuclear Physics, Polish Academy of Science, ul. Radzikowskiego 152, PL-31342 Kraków, Poland.

Instituto de Física, Universidad Nacional Autónoma de México, Apdo. Postal 20-364, Ciudad de México 01000, Mexico.

出版信息

Entropy (Basel). 2024 Aug 5;26(8):665. doi: 10.3390/e26080665.

DOI:10.3390/e26080665
PMID:39202135
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11353880/
Abstract

We consider two different time fractional telegrapher's equations under stochastic resetting. Using the integral decomposition method, we found the probability density functions and the mean squared displacements. In the long-time limit, the system approaches non-equilibrium stationary states, while the mean squared displacement saturates due to the resetting mechanism. We also obtain the fractional telegraph process as a subordinated telegraph process by introducing operational time such that the physical time is considered as a Lévy stable process whose characteristic function is the Lévy stable distribution. We also analyzed the survival probability for the first-passage time problem and found the optimal resetting rate for which the corresponding mean first-passage time is minimal.

摘要

我们考虑了随机重置下的两种不同的时间分数阶电报方程。使用积分分解方法,我们得到了概率密度函数和均方位移。在长时间极限下,系统趋近于非平衡稳态,而由于重置机制,均方位移会饱和。通过引入运算时间,使得物理时间被视为具有特征函数为 Lévy 稳定分布的 Lévy 稳定过程,我们还得到了作为从属电报过程的分数阶电报过程。我们还分析了首通时间问题的生存概率,并找到了相应的平均首通时间最小的最优重置率。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/30a2ad1e7b63/entropy-26-00665-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/9a59150960c3/entropy-26-00665-g0A1.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/1202e0870e53/entropy-26-00665-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/deac69c6d716/entropy-26-00665-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/3da9bf9e8b64/entropy-26-00665-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/f83642b7be89/entropy-26-00665-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/30a2ad1e7b63/entropy-26-00665-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/9a59150960c3/entropy-26-00665-g0A1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/7c89540bc2c2/entropy-26-00665-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/1202e0870e53/entropy-26-00665-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/deac69c6d716/entropy-26-00665-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/3da9bf9e8b64/entropy-26-00665-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/f83642b7be89/entropy-26-00665-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/426c/11353880/30a2ad1e7b63/entropy-26-00665-g006.jpg

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Phys Rev E. 2021 Aug;104(2-1):024113. doi: 10.1103/PhysRevE.104.024113.