Deep glassy state dynamic data challenge glass models: Elastic models

There is increasing experimental evidence that suggests that the dynamics of glass forming liquids do not diverge at finite temperature above zero Kelvin, at the same time there has been recent progress in the development of non-diverging glass transition models. In this work we examine two non-dive...

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Main Authors: Dongjie Chen, Gregory B. McKenna
Format: Article
Language:English
Published: Elsevier 2021-09-01
Series:Journal of Non-Crystalline Solids: X
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S2590159121000091
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spelling doaj-45bcbd95bb314984817ae1f6bccac5b42021-10-01T05:10:51ZengElsevierJournal of Non-Crystalline Solids: X2590-15912021-09-0111100068Deep glassy state dynamic data challenge glass models: Elastic modelsDongjie Chen0Gregory B. McKenna1Department of Chemical Engineering, Texas Tech University, Lubbock, TX 79409, United States of AmericaDepartment of Chemical Engineering, Texas Tech University, Lubbock, TX 79409, United States of America; Department of Chemical and Biomolecular Engineering, North Carolina State University, Raleigh, NC 27695, United States of America; Corresponding author at: Department of Chemical Engineering, Texas Tech University, Lubbock, TX 79409, United States of America.There is increasing experimental evidence that suggests that the dynamics of glass forming liquids do not diverge at finite temperature above zero Kelvin, at the same time there has been recent progress in the development of non-diverging glass transition models. In this work we examine two non-diverging models: the elastically collective nonlinear Langevin equation theory (ECNLE) and the shoving model, both of which relate an energy barrier in the glass formation process with elastic motion at small scales. The models are evaluated in comparison with the non-diverging dynamic data obtained in the deep glassy state (very stable) for a 20-million-year-old (20 Ma) ancient amber and for a vapor deposited amorphous Teflon obtained previously. We find that although both models are in qualitative agreement with the dynamic data for the two stable glasses, they still overestimate the actual relaxation times for the deep glassy state below the nominal glass transition temperature and for conditions corresponding to the equilibrium state or in a state in which the glass relaxation times are upper bounds to the equilibrium values.http://www.sciencedirect.com/science/article/pii/S2590159121000091Glass transitionDiverging time-scalesNon-diverging time-scalesECNLE modelShoving modelGlass dynamics
collection DOAJ
language English
format Article
sources DOAJ
author Dongjie Chen
Gregory B. McKenna
spellingShingle Dongjie Chen
Gregory B. McKenna
Deep glassy state dynamic data challenge glass models: Elastic models
Journal of Non-Crystalline Solids: X
Glass transition
Diverging time-scales
Non-diverging time-scales
ECNLE model
Shoving model
Glass dynamics
author_facet Dongjie Chen
Gregory B. McKenna
author_sort Dongjie Chen
title Deep glassy state dynamic data challenge glass models: Elastic models
title_short Deep glassy state dynamic data challenge glass models: Elastic models
title_full Deep glassy state dynamic data challenge glass models: Elastic models
title_fullStr Deep glassy state dynamic data challenge glass models: Elastic models
title_full_unstemmed Deep glassy state dynamic data challenge glass models: Elastic models
title_sort deep glassy state dynamic data challenge glass models: elastic models
publisher Elsevier
series Journal of Non-Crystalline Solids: X
issn 2590-1591
publishDate 2021-09-01
description There is increasing experimental evidence that suggests that the dynamics of glass forming liquids do not diverge at finite temperature above zero Kelvin, at the same time there has been recent progress in the development of non-diverging glass transition models. In this work we examine two non-diverging models: the elastically collective nonlinear Langevin equation theory (ECNLE) and the shoving model, both of which relate an energy barrier in the glass formation process with elastic motion at small scales. The models are evaluated in comparison with the non-diverging dynamic data obtained in the deep glassy state (very stable) for a 20-million-year-old (20 Ma) ancient amber and for a vapor deposited amorphous Teflon obtained previously. We find that although both models are in qualitative agreement with the dynamic data for the two stable glasses, they still overestimate the actual relaxation times for the deep glassy state below the nominal glass transition temperature and for conditions corresponding to the equilibrium state or in a state in which the glass relaxation times are upper bounds to the equilibrium values.
topic Glass transition
Diverging time-scales
Non-diverging time-scales
ECNLE model
Shoving model
Glass dynamics
url http://www.sciencedirect.com/science/article/pii/S2590159121000091
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AT gregorybmckenna deepglassystatedynamicdatachallengeglassmodelselasticmodels
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