Self-diffusion anomalies of an odd tracer in soft-core media

Odd-diffusive systems, characterised by broken time-reversal and/or parity, have recently been shown to display counterintuitive features such as interaction-enhanced dynamics in the dilute limit. Here we extend the investigation to the high-density limit of an odd tracer embedded in a soft medium d...

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Main Authors: Pietro Luigi Muzzeddu, Erik Kalz, Andrea Gambassi, Abhinav Sharma, Ralf Metzler
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:New Journal of Physics
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Online Access:https://doi.org/10.1088/1367-2630/adbdea
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author Pietro Luigi Muzzeddu
Erik Kalz
Andrea Gambassi
Abhinav Sharma
Ralf Metzler
author_facet Pietro Luigi Muzzeddu
Erik Kalz
Andrea Gambassi
Abhinav Sharma
Ralf Metzler
author_sort Pietro Luigi Muzzeddu
collection DOAJ
description Odd-diffusive systems, characterised by broken time-reversal and/or parity, have recently been shown to display counterintuitive features such as interaction-enhanced dynamics in the dilute limit. Here we extend the investigation to the high-density limit of an odd tracer embedded in a soft medium described by the Gaussian core model (GCM) using a field-theoretic approach based on the Dean–Kawasaki equation. Our analysis reveals that interactions can enhance the dynamics of an odd tracer even in dense systems. We demonstrate that oddness results in a complete reversal of the well-known self-diffusion ( $D_\mathrm{s}$ ) anomaly of the GCM. Ordinarily, $D_\mathrm{s}$ exhibits a non-monotonic trend with increasing density, approaching but remaining below the interaction-free diffusion, D _0 , ( $D_\mathrm{s} \lt D_0$ ) so that $D_\mathrm{s} \uparrow D_0$ at high densities. In contrast, for an odd tracer, self-diffusion is enhanced ( $D_\mathrm{s} \gt D_0$ ) and the GCM anomaly is inverted, displaying $D_\mathrm{s} \downarrow D_0$ at high densities. The transition between the standard and reversed GCM anomaly is governed by the tracer’s oddness, with a critical oddness value at which the tracer diffuses as a free particle ( $D_\mathrm{s} \approx D_0$ ) across all densities. We validate our theoretical predictions with Brownian dynamics simulations, finding strong agreement between the them.
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spelling doaj-art-17fbfc445a114e54891e82a11cede65f2025-08-20T02:10:42ZengIOP PublishingNew Journal of Physics1367-26302025-01-0127303302510.1088/1367-2630/adbdeaSelf-diffusion anomalies of an odd tracer in soft-core mediaPietro Luigi Muzzeddu0https://orcid.org/0000-0002-1059-8240Erik Kalz1https://orcid.org/0000-0003-3294-7365Andrea Gambassi2https://orcid.org/0000-0003-3450-6125Abhinav Sharma3https://orcid.org/0000-0002-6436-3826Ralf Metzler4https://orcid.org/0000-0002-6013-7020Department of Biochemistry, University of Geneva , CH-1211 Geneva, SwitzerlandUniversity of Potsdam, Institute of Physics and Astronomy , D-14476 Potsdam, GermanySISSA—International School for Advanced Studies , IT-34136 Trieste, Italy; INFN—Sezione di Trieste , IT-34127 Trieste, ItalyUniversity of Augsburg , Institute of Physics, D-86159 Augsburg, Germany; Leibniz-Institute for Polymer Research, Institute Theory of Polymers , D-01069 Dresden, GermanyUniversity of Potsdam, Institute of Physics and Astronomy , D-14476 Potsdam, Germany; Asia Pacific Centre for Theoretical Physics , KR-37673 Pohang, Republic of KoreaOdd-diffusive systems, characterised by broken time-reversal and/or parity, have recently been shown to display counterintuitive features such as interaction-enhanced dynamics in the dilute limit. Here we extend the investigation to the high-density limit of an odd tracer embedded in a soft medium described by the Gaussian core model (GCM) using a field-theoretic approach based on the Dean–Kawasaki equation. Our analysis reveals that interactions can enhance the dynamics of an odd tracer even in dense systems. We demonstrate that oddness results in a complete reversal of the well-known self-diffusion ( $D_\mathrm{s}$ ) anomaly of the GCM. Ordinarily, $D_\mathrm{s}$ exhibits a non-monotonic trend with increasing density, approaching but remaining below the interaction-free diffusion, D _0 , ( $D_\mathrm{s} \lt D_0$ ) so that $D_\mathrm{s} \uparrow D_0$ at high densities. In contrast, for an odd tracer, self-diffusion is enhanced ( $D_\mathrm{s} \gt D_0$ ) and the GCM anomaly is inverted, displaying $D_\mathrm{s} \downarrow D_0$ at high densities. The transition between the standard and reversed GCM anomaly is governed by the tracer’s oddness, with a critical oddness value at which the tracer diffuses as a free particle ( $D_\mathrm{s} \approx D_0$ ) across all densities. We validate our theoretical predictions with Brownian dynamics simulations, finding strong agreement between the them.https://doi.org/10.1088/1367-2630/adbdeainteracting colloidsodd diffusionDean–Kawasaki equationstochastic field theoryself-diffusion anomalyGaussian core model
spellingShingle Pietro Luigi Muzzeddu
Erik Kalz
Andrea Gambassi
Abhinav Sharma
Ralf Metzler
Self-diffusion anomalies of an odd tracer in soft-core media
New Journal of Physics
interacting colloids
odd diffusion
Dean–Kawasaki equation
stochastic field theory
self-diffusion anomaly
Gaussian core model
title Self-diffusion anomalies of an odd tracer in soft-core media
title_full Self-diffusion anomalies of an odd tracer in soft-core media
title_fullStr Self-diffusion anomalies of an odd tracer in soft-core media
title_full_unstemmed Self-diffusion anomalies of an odd tracer in soft-core media
title_short Self-diffusion anomalies of an odd tracer in soft-core media
title_sort self diffusion anomalies of an odd tracer in soft core media
topic interacting colloids
odd diffusion
Dean–Kawasaki equation
stochastic field theory
self-diffusion anomaly
Gaussian core model
url https://doi.org/10.1088/1367-2630/adbdea
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