Ideal Shear Strength Of A Quantum Crystal

dc.creatorBorda E.J.L.
dc.creatorCai W.
dc.creatorDe Koning M.
dc.date2014
dc.date2015-06-25T18:00:52Z
dc.date2015-11-26T15:02:19Z
dc.date2015-06-25T18:00:52Z
dc.date2015-11-26T15:02:19Z
dc.date.accessioned2018-03-28T22:13:15Z
dc.date.available2018-03-28T22:13:15Z
dc.identifier
dc.identifierPhysical Review Letters. American Physical Society, v. 112, n. 15, p. - , 2014.
dc.identifier319007
dc.identifier10.1103/PhysRevLett.112.155303
dc.identifierhttp://www.scopus.com/inward/record.url?eid=2-s2.0-84899027735&partnerID=40&md5=40a503f7f7a70b317aefc1f26469a99a
dc.identifierhttp://www.repositorio.unicamp.br/handle/REPOSIP/87437
dc.identifierhttp://repositorio.unicamp.br/jspui/handle/REPOSIP/87437
dc.identifier2-s2.0-84899027735
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1256434
dc.descriptionUsing path-integral Monte Carlo simulations, we compute the ideal shear strength (ISS) on the basal plane of hcp He4. The failure mode upon reaching the ISS limit is characterized by the homogeneous nucleation of a stacking fault and it is found to be anisotropic, consistent with Schmid's law of resolved shear stress. Comparing the ISS of hcp He4 to a large set of classical crystals shows that it closely fits the approximately universal modified Frenkel model of ideal strength. In addition to giving quantitative stress levels for the homogeneous nucleation of extended defects in hcp He4, our findings lend support to assumptions in the literature that inherently classical models remain useful for the description of mechanical behavior in quantum crystals. © 2014 American Physical Society.
dc.description112
dc.description15
dc.description
dc.description
dc.descriptionBES; Office of Basic Energy Sciences
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dc.languageen
dc.publisherAmerican Physical Society
dc.relationPhysical Review Letters
dc.rightsaberto
dc.sourceScopus
dc.titleIdeal Shear Strength Of A Quantum Crystal
dc.typeArtículos de revistas


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