Glass Forming Ability in Systems with Competing Orderings
Some liquids, if cooled rapidly enough to avoid crystallization, can be frozen into a nonergodic glassy state. The tendency for a material to form a glass when quenched is called “glass-forming ability,” and it is of key significance both fundamentally and for materials science applications. Here, w...
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2018-05-01
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Series: | Physical Review X |
Online Access: | http://doi.org/10.1103/PhysRevX.8.021040 |
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doaj-79c866ba4808417aae476032461431e32020-11-24T20:44:34ZengAmerican Physical SocietyPhysical Review X2160-33082018-05-018202104010.1103/PhysRevX.8.021040Glass Forming Ability in Systems with Competing OrderingsJohn RussoFlavio RomanoHajime TanakaSome liquids, if cooled rapidly enough to avoid crystallization, can be frozen into a nonergodic glassy state. The tendency for a material to form a glass when quenched is called “glass-forming ability,” and it is of key significance both fundamentally and for materials science applications. Here, we consider liquids with competing orderings, where an increase in the glass-forming ability is signaled by a depression of the melting temperature towards its minimum at triple or eutectic points. With simulations of two model systems where glass-forming ability can be tuned by an external parameter, we are able to interpolate between crystal-forming and glass-forming behavior. We find that the enhancement of the glass-forming ability is caused by an increase in the structural difference between liquid and crystal: stronger competition in orderings towards the melting point minimum makes a liquid structure more disordered (more complex). This increase in the liquid-crystal structure difference can be described by a single adimensional parameter, i.e., the interface energy cost scaled by the thermal energy, which we call the “thermodynamic interface penalty.” Our finding may provide a general physical principle for not only controlling the glass-forming ability but also the emergence of glassy behavior of various systems with competing orderings, including orderings of structural, magnetic, electronic, charge, and dipolar origin.http://doi.org/10.1103/PhysRevX.8.021040 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
John Russo Flavio Romano Hajime Tanaka |
spellingShingle |
John Russo Flavio Romano Hajime Tanaka Glass Forming Ability in Systems with Competing Orderings Physical Review X |
author_facet |
John Russo Flavio Romano Hajime Tanaka |
author_sort |
John Russo |
title |
Glass Forming Ability in Systems with Competing Orderings |
title_short |
Glass Forming Ability in Systems with Competing Orderings |
title_full |
Glass Forming Ability in Systems with Competing Orderings |
title_fullStr |
Glass Forming Ability in Systems with Competing Orderings |
title_full_unstemmed |
Glass Forming Ability in Systems with Competing Orderings |
title_sort |
glass forming ability in systems with competing orderings |
publisher |
American Physical Society |
series |
Physical Review X |
issn |
2160-3308 |
publishDate |
2018-05-01 |
description |
Some liquids, if cooled rapidly enough to avoid crystallization, can be frozen into a nonergodic glassy state. The tendency for a material to form a glass when quenched is called “glass-forming ability,” and it is of key significance both fundamentally and for materials science applications. Here, we consider liquids with competing orderings, where an increase in the glass-forming ability is signaled by a depression of the melting temperature towards its minimum at triple or eutectic points. With simulations of two model systems where glass-forming ability can be tuned by an external parameter, we are able to interpolate between crystal-forming and glass-forming behavior. We find that the enhancement of the glass-forming ability is caused by an increase in the structural difference between liquid and crystal: stronger competition in orderings towards the melting point minimum makes a liquid structure more disordered (more complex). This increase in the liquid-crystal structure difference can be described by a single adimensional parameter, i.e., the interface energy cost scaled by the thermal energy, which we call the “thermodynamic interface penalty.” Our finding may provide a general physical principle for not only controlling the glass-forming ability but also the emergence of glassy behavior of various systems with competing orderings, including orderings of structural, magnetic, electronic, charge, and dipolar origin. |
url |
http://doi.org/10.1103/PhysRevX.8.021040 |
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