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Relating fragile-to-strong transition to fragile glass via lattice model simulations.
Ong, Chin-Yuan; Lee, Chun-Shing; Gao, Xin-Yuan; Zhai, Qiang; Yu, Zhenhao; Shi, Rui; Deng, Hai-Yao; Lam, Chi-Hang.
Affiliation
  • Ong CY; Department of Applied Physics, Hong Kong Polytechnic University, Hong Kong, China.
  • Lee CS; Department of Applied Physics, Hong Kong Polytechnic University, Hong Kong, China.
  • Gao XY; School of Science, Harbin Institute of Technology (Shenzhen), Shenzhen 518055, China.
  • Zhai Q; Department of Applied Physics, Hong Kong Polytechnic University, Hong Kong, China.
  • Yu Z; School of Physics, MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, Xi'an Jiaotong University, Xi'an 710049, China.
  • Shi R; Zhejiang Key Laboratory of Micro-nano Quantum Chips and Quantum Control, School of Physics, Zhejiang University, Hangzhou 310027, China.
  • Deng HY; Zhejiang Key Laboratory of Micro-nano Quantum Chips and Quantum Control, School of Physics, Zhejiang University, Hangzhou 310027, China.
  • Lam CH; School of Physics and Astronomy, Cardiff University, 5 The Parade, Cardiff CF24 3AA, Wales, United Kingdom.
Phys Rev E ; 109(5-1): 054124, 2024 May.
Article in En | MEDLINE | ID: mdl-38907442
ABSTRACT
Glass formers are, in general, classified as strong or fragile depending on whether their relaxation rates follow Arrhenius or super-Arrhenius temperature dependence. There are, however, notable exceptions, such as water, which exhibit a fragile-to-strong (FTS) transition and behave as fragile and strong, respectively, at high and low temperatures. In this work, the FTS transition is studied using a distinguishable-particle lattice model previously demonstrated to be capable of simulating both strong and fragile glasses [C.-S. Lee, M. Lulli, L.-H. Zhang, H.-Y. Deng, and C.-H. Lam, Phys. Rev. Lett. 125, 265703 (2020)0031-900710.1103/PhysRevLett.125.265703]. Starting with a bimodal pair-interaction distribution appropriate for fragile glasses, we show that by narrowing down the energy dispersion in the low-energy component of the distribution, a FTS transition is observed. The transition occurs at a temperature at which the stretching exponent of the relaxation is minimized, in agreement with previous molecular dynamics simulations.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev E Year: 2024 Document type: Article Affiliation country: China

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev E Year: 2024 Document type: Article Affiliation country: China