Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/6232
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dc.contributorDepartment of Applied Physics-
dc.creatorWu, RPH-
dc.creatorLo, VC-
dc.creatorHuang, H-
dc.date.accessioned2014-12-11T08:22:30Z-
dc.date.available2014-12-11T08:22:30Z-
dc.identifier.issn0021-8979-
dc.identifier.urihttp://hdl.handle.net/10397/6232-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2012 American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics. The following article appeared in R. P. H. Wu et al., J. Appl. Phys. 112, 063924 (2012) and may be found at http://link.aip.org/link/?jap/112/063924.en_US
dc.subjectCritical exponentsen_US
dc.subjectGaussian distributionen_US
dc.subjectIsing modelen_US
dc.subjectKosterlitz-Thouless transitionen_US
dc.subjectMagnetic transitionsen_US
dc.subjectMonte Carlo methodsen_US
dc.subjectOrder-disorder transformationsen_US
dc.subjectSpin systemsen_US
dc.titleCritical behavior of two-dimensional spin systems under the random-bond six-state clock modelen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1-
dc.identifier.epage8-
dc.identifier.volume112-
dc.identifier.issue6-
dc.identifier.doi10.1063/1.4754821-
dcterms.abstractThe critical behavior of the clock model in two-dimensional square lattice is studied numerically using Monte Carlo method with Wolff algorithm. The Kosterlitz-Thouless (KT) transition is observed in the six-state clock model, where an intermediate phase exists between the low-temperature ordered phase and the high-temperature disordered phase. The bond randomness is introduced to the system by assuming a Gaussian distribution for the coupling coefficients with the mean μ = 1 and different values of variance, from σ² = 0.1 to σ² = 3.0. An abrupt jump in the helicity modulus at the transition, which is the key characteristic of the KT transition, is verified with a stability argument. The critical temperature T[sub c] for both pure and disordered systems is determined from the critical exponent η(T[sub c]) = 1/4. The results showed that a small amount of disorder (small σ) reduces the critical temperature of the system, without altering the nature of transition. However, a larger amount of disorder changes the transition from the KT-type into that of non-KT-type.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 15 Sept. 2012, v. 112, no. 6, 063924 , p. 1-8-
dcterms.isPartOfJournal of applied physics-
dcterms.issued2012-09-15-
dc.identifier.isiWOS:000309423200096-
dc.identifier.scopus2-s2.0-84867075042-
dc.identifier.eissn1089-7550-
dc.identifier.rosgroupidr63387-
dc.description.ros2012-2013 > Academic research: refereed > Publication in refereed journal-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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