Dynamic phase coexistence in glass–forming liquids

One of the most controversial hypotheses for explaining the heterogeneous dynamics of glasses postulates the temporary coexistence of two phases characterized by a high and by a low diffusivity. In this scenario, two phases with different diffusivities coexist for a time of the order of the relaxati...

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Main Authors: Pastore, Raffaele, Coniglio, Antonio, Ciamarra, Massimo Pica
Other Authors: School of Physical and Mathematical Sciences
Format: Article
Language:English
Published: 2015
Online Access:https://hdl.handle.net/10356/103361
http://hdl.handle.net/10220/38733
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Institution: Nanyang Technological University
Language: English
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spelling sg-ntu-dr.10356-1033612023-02-28T19:21:45Z Dynamic phase coexistence in glass–forming liquids Pastore, Raffaele Coniglio, Antonio Ciamarra, Massimo Pica School of Physical and Mathematical Sciences One of the most controversial hypotheses for explaining the heterogeneous dynamics of glasses postulates the temporary coexistence of two phases characterized by a high and by a low diffusivity. In this scenario, two phases with different diffusivities coexist for a time of the order of the relaxation time and mix afterwards. Unfortunately, it is difficult to measure the single-particle diffusivities to test this hypothesis. Indeed, although the non-Gaussian shape of the van-Hove distribution suggests the transient existence of a diffusivity distribution, it is not possible to infer from this quantity whether two or more dynamical phases coexist. Here we provide the first direct observation of the dynamical coexistence of two phases with different diffusivities, by showing that in the deeply supercooled regime the distribution of the single-particle diffusivities acquires a transient bimodal shape. We relate this distribution to the heterogeneity of the dynamics and to the breakdown of the Stokes-Einstein relation, and we show that the coexistence of two dynamical phases occurs up to a timescale growing faster than the relaxation time on cooling, for some of the considered models. Our work offers a basis for rationalizing the dynamics of supercooled liquids and for relating their structural and dynamical properties. Published version 2015-09-23T03:48:12Z 2019-12-06T21:10:55Z 2015-09-23T03:48:12Z 2019-12-06T21:10:55Z 2015 2015 Journal Article Pastore, R., Coniglio, A., & Ciamarra, M. P. (2015). Dynamic phase coexistence in glass–forming liquids. Scientific Reports, 5, 11770-. 2045-2322 https://hdl.handle.net/10356/103361 http://hdl.handle.net/10220/38733 10.1038/srep11770 26156304 en Scientific Reports This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ application/pdf
institution Nanyang Technological University
building NTU Library
continent Asia
country Singapore
Singapore
content_provider NTU Library
collection DR-NTU
language English
description One of the most controversial hypotheses for explaining the heterogeneous dynamics of glasses postulates the temporary coexistence of two phases characterized by a high and by a low diffusivity. In this scenario, two phases with different diffusivities coexist for a time of the order of the relaxation time and mix afterwards. Unfortunately, it is difficult to measure the single-particle diffusivities to test this hypothesis. Indeed, although the non-Gaussian shape of the van-Hove distribution suggests the transient existence of a diffusivity distribution, it is not possible to infer from this quantity whether two or more dynamical phases coexist. Here we provide the first direct observation of the dynamical coexistence of two phases with different diffusivities, by showing that in the deeply supercooled regime the distribution of the single-particle diffusivities acquires a transient bimodal shape. We relate this distribution to the heterogeneity of the dynamics and to the breakdown of the Stokes-Einstein relation, and we show that the coexistence of two dynamical phases occurs up to a timescale growing faster than the relaxation time on cooling, for some of the considered models. Our work offers a basis for rationalizing the dynamics of supercooled liquids and for relating their structural and dynamical properties.
author2 School of Physical and Mathematical Sciences
author_facet School of Physical and Mathematical Sciences
Pastore, Raffaele
Coniglio, Antonio
Ciamarra, Massimo Pica
format Article
author Pastore, Raffaele
Coniglio, Antonio
Ciamarra, Massimo Pica
spellingShingle Pastore, Raffaele
Coniglio, Antonio
Ciamarra, Massimo Pica
Dynamic phase coexistence in glass–forming liquids
author_sort Pastore, Raffaele
title Dynamic phase coexistence in glass–forming liquids
title_short Dynamic phase coexistence in glass–forming liquids
title_full Dynamic phase coexistence in glass–forming liquids
title_fullStr Dynamic phase coexistence in glass–forming liquids
title_full_unstemmed Dynamic phase coexistence in glass–forming liquids
title_sort dynamic phase coexistence in glass–forming liquids
publishDate 2015
url https://hdl.handle.net/10356/103361
http://hdl.handle.net/10220/38733
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