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Evidence for a spinodal limit of amorphous excitations in glassy systems

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C Cammarota1,2, A Cavagna2,3, G Gradenigo4,5, T S Grigera6,7 and P Verrocchio4,5,8

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LETTER

What is the origin of the sharp slowdown displayed by glassy systems? Physical common sense suggests there must be a concomitant growing correlation length, but finding this length has been nontrivial. In random first-order theory, it is given by the size of amorphous excitations, which depends on a balance between their mutual interfacial energy and their configurational entropy. But how these excitations disappear when crossing over to the normal high temperature phase is unclear, chiefly due to lack of data about the surface tension. We measure the energy cost for creating amorphous excitations in a model glass-former, and discover that the surface tension vanishes at a well-defined spinodal energy, above which amorphous excitations cannot be sustained. This spinodal therefore marks the true onset of glassiness.


Keywords

energy landscapes (theory)

structural glasses (theory)

disordered systems (theory)

PACS

61.43.Fs Glasses

64.70.P- Glass transitions of specific systems

64.70.D- Solid–liquid transitions

68.03.Cd Surface tension and related phenomena

65.60.+a Thermal properties of amorphous solids and glasses: heat capacity, thermal expansion, etc.

MSC

82C44 Dynamics of disordered systems (random Ising systems, etc.)

82C26 Dynamic and nonequilibrium phase transitions (general)

82D30 Random media, disordered materials (including liquid crystals and spin glasses)

82C35 Irreversible thermodynamics, including Onsager-Machlup theory

Subjects

Soft matter, liquids and polymers

Surfaces, interfaces and thin films

Condensed matter: structural, mechanical & thermal

Dates

Issue 12 (December 2009)

Received 22 September 2009, accepted for publication 3 December 2009

Published 21 December 2009



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