Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/107632
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dc.contributorDepartment of Applied Physicsen_US
dc.creatorOng, CYen_US
dc.creatorLee, CSen_US
dc.creatorGao, XYen_US
dc.creatorZhai, Qen_US
dc.creatorYu, Zen_US
dc.creatorShi, Ren_US
dc.creatorDeng, HYen_US
dc.creatorLam, CHen_US
dc.date.accessioned2024-07-05T07:15:12Z-
dc.date.available2024-07-05T07:15:12Z-
dc.identifier.issn2470-0045,en_US
dc.identifier.urihttp://hdl.handle.net/10397/107632-
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.rights©2024 American Physical Societyen_US
dc.rightsThe following publication Ong, C.-Y., Lee, C.-S., Gao, X.-Y., Zhai, Q., Yu, Z., Shi, R., Deng, H.-Y., & Lam, C.-H. (2024). Relating fragile-to-strong transition to fragile glass via lattice model simulations. Physical Review E, 109(5), 054124 is available at https://doi.org/10.1103/PhysRevE.109.054124.en_US
dc.titleRelating fragile-to-strong transition to fragile glass via lattice model simulationsen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume109en_US
dc.identifier.issue5en_US
dc.identifier.doi10.1103/PhysRevE.109.054124en_US
dcterms.abstractGlass 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)]. 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.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationPhysical review E : covering statistical, nonlinear, biological, and soft matter physics, May 2024, v. 109, no. 5, 054124en_US
dcterms.isPartOfPhysical review E : covering statistical, nonlinear, biological, and soft matter physicsen_US
dcterms.issued2024-05-
dc.identifier.scopus2-s2.0-85194927801-
dc.identifier.eissn2470-0053en_US
dc.identifier.artn054124en_US
dc.description.validate202407 bcchen_US
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumbera2957-
dc.identifier.SubFormID48928-
dc.description.fundingSourceRGCen_US
dc.description.pubStatusPublisheden_US
dc.description.oaCategoryVoR alloweden_US
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