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Auteurs principaux: Hislop, Peter D., Soccorsi, Eric
Format: Preprint
Publié: 2024
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Accès en ligne:https://arxiv.org/abs/2401.07117
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author Hislop, Peter D.
Soccorsi, Eric
author_facet Hislop, Peter D.
Soccorsi, Eric
contents We study the large-time asymptotics of the edge current for a family of time-fractional Schrodinger equations with a constant, transverse magnetic field on a half-plane $(x,y) \in \mathbb{R}_x^+ \times \mathbb{R}_y$. The TFSE is parameterized by two constants $(α, β)$ in $(0,1]$, where $α$ is the fractional order of the time derivative, and $β$ is the power of $i$ in the Schrodinger equation. We prove that for fixed $α$, there is a transition in the transport properties as $β$ varies in $(0,1]$: For $0 < β< α$, the edge current grows exponentially in time, for $α= β$, the edge current is asymptotically constant, and for $β> α$, the edge current decays in time. We prove that the mean square displacement in the $y\in \mathbb{R}$-direction undergoes a similar transport transition. These results provide quantitative support for the comments of Laskin \cite{laskin2000_1} that the latter two cases, $α= β$ and $α< β$, are the physically relevant ones.
format Preprint
id arxiv_https___arxiv_org_abs_2401_07117
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Edge currents for the time-fractional, half-plane, Schrodinger equation with constant magnetic field
Hislop, Peter D.
Soccorsi, Eric
Mathematical Physics
35Q40 35R11 81Q99
We study the large-time asymptotics of the edge current for a family of time-fractional Schrodinger equations with a constant, transverse magnetic field on a half-plane $(x,y) \in \mathbb{R}_x^+ \times \mathbb{R}_y$. The TFSE is parameterized by two constants $(α, β)$ in $(0,1]$, where $α$ is the fractional order of the time derivative, and $β$ is the power of $i$ in the Schrodinger equation. We prove that for fixed $α$, there is a transition in the transport properties as $β$ varies in $(0,1]$: For $0 < β< α$, the edge current grows exponentially in time, for $α= β$, the edge current is asymptotically constant, and for $β> α$, the edge current decays in time. We prove that the mean square displacement in the $y\in \mathbb{R}$-direction undergoes a similar transport transition. These results provide quantitative support for the comments of Laskin \cite{laskin2000_1} that the latter two cases, $α= β$ and $α< β$, are the physically relevant ones.
title Edge currents for the time-fractional, half-plane, Schrodinger equation with constant magnetic field
topic Mathematical Physics
35Q40 35R11 81Q99
url https://arxiv.org/abs/2401.07117