Glass transition, topology, and elastic models of Se‐based glasses

Author:

Chbeir Ralph1,Welton Aaron1,Burger Matthew1,Chakravarty Soumendu2,Dash Shreeram2,Bhosle Siddhesh1,Gunasekera Kapila1,Almutairi Badriah S.3,Goodman Bernard3,Micoulaut Matthieu4,Boolchand Punit1ORCID

Affiliation:

1. Department of Electrical Engineering and Computer Science University of Cincinnati Cincinnati Ohio USA

2. Department of Department of Mechanical and Materials Engineering University of Cincinnati Cincinnati Ohio USA

3. Department of Physics University of Cincinnati Cincinnati Ohio USA

4. Laboratoire de Physique Théorique de la Matière Condensée CNRS UMR 7600 Sorbonne Université Paris France

Abstract

AbstractFeatures intrinsic to disorder and network aspects are ubiquitous in structural glasses. Among this important class of materials, chalcogenide glasses are special—they are built of short‐range covalent forces, making them simpler than silicate glasses that possess mixed ionic and covalent forces. Selenium‐based glasses also display complex elastic phase transitions that have been described from various models, including mean‐field approaches to molecular simulations. These point to the presence of two sharply defined elastic phase transitions, a rigidity and stress transition that are non‐mean‐field in character, and separate the three distinct topological phases of flexible, isostatically rigid, and stressed‐rigid. This article reviews the physics of these glassy networks. The elastic phases and glass transition temperature are explained on a molecular level in terms of topological constraint theory (TCT), connectivity, and the open degrees of freedom. The broader aspects of TCT in relation to phase change materials, high‐k dielectrics, and cements are also commented upon.

Funder

National Science Foundation

Publisher

Wiley

Subject

Materials Chemistry,Ceramics and Composites

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