Planckian Diffusion: The Ghost of Anderson Localization

Fuente: arXiv
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Main Authors: Zhang, Yubo, Graf, Anton M., Aydin, Alhun, Keski-Rahkonen, Joonas, Heller, Eric J.
Format: Preprint
Published: 2024
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_version_ 1866916497943691264
author Zhang, Yubo
Graf, Anton M.
Aydin, Alhun
Keski-Rahkonen, Joonas
Heller, Eric J.
author_facet Zhang, Yubo
Graf, Anton M.
Aydin, Alhun
Keski-Rahkonen, Joonas
Heller, Eric J.
contents We find that Anderson localization ceases to exist when a random medium begins to move, but another type of fundamental quantum effect, Planckian diffusion $D = α\hbar/m$, rises to replace it, with $α$ of order of unity. Planckian diffusion supercedes the Planckian speed limit $τ= α\hbar/k_B T,$ as it not only implies this relation in thermal systems but also applies more generally without requiring thermal equilibrium. Here we model a dynamic disordered system with thousands of itinerant impurities, having random initial positions and velocities. By incrementally increasing their speed from zero, we observe a transition from Anderson localization to Planckian diffusion, with $α$ falling within the range of $0.5$ to $2$. Furthermore, we relate the breakdown of Anderson localization to three additional, distinctly different confirming cases that also exhibit Planckian diffusion $D\sim \hbar/m$, including one experiment on solid hydrogen. Our finding suggests that Planckian diffusion in dynamic disordered systems is as universal as Anderson localization in static disordered systems, which may shed light on quantum transport studies.
format Preprint
id arxiv_https___arxiv_org_abs_2411_18768
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Planckian Diffusion: The Ghost of Anderson Localization
Zhang, Yubo
Graf, Anton M.
Aydin, Alhun
Keski-Rahkonen, Joonas
Heller, Eric J.
Quantum Physics
Disordered Systems and Neural Networks
We find that Anderson localization ceases to exist when a random medium begins to move, but another type of fundamental quantum effect, Planckian diffusion $D = α\hbar/m$, rises to replace it, with $α$ of order of unity. Planckian diffusion supercedes the Planckian speed limit $τ= α\hbar/k_B T,$ as it not only implies this relation in thermal systems but also applies more generally without requiring thermal equilibrium. Here we model a dynamic disordered system with thousands of itinerant impurities, having random initial positions and velocities. By incrementally increasing their speed from zero, we observe a transition from Anderson localization to Planckian diffusion, with $α$ falling within the range of $0.5$ to $2$. Furthermore, we relate the breakdown of Anderson localization to three additional, distinctly different confirming cases that also exhibit Planckian diffusion $D\sim \hbar/m$, including one experiment on solid hydrogen. Our finding suggests that Planckian diffusion in dynamic disordered systems is as universal as Anderson localization in static disordered systems, which may shed light on quantum transport studies.
title Planckian Diffusion: The Ghost of Anderson Localization
topic Quantum Physics
Disordered Systems and Neural Networks
url https://arxiv.org/abs/2411.18768