Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/23728
DC FieldValueLanguage
dc.contributorDepartment of Applied Mathematics-
dc.creatorLi, XG-
dc.creatorChan, CK-
dc.creatorHou, Y-
dc.date.accessioned2015-03-30T06:30:51Z-
dc.date.available2015-03-30T06:30:51Z-
dc.identifier.issn0096-3003-
dc.identifier.urihttp://hdl.handle.net/10397/23728-
dc.language.isoenen_US
dc.publisherElsevieren_US
dc.subjectConservationen_US
dc.subjectDynamicsen_US
dc.subjectFinite differenceen_US
dc.subjectMaxwell-Dirac systemen_US
dc.subjectTime-splitting methoden_US
dc.titleA numerical method with particle conservation for the Maxwell-Dirac systemen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1096-
dc.identifier.epage1108-
dc.identifier.volume216-
dc.identifier.issue4-
dc.identifier.doi10.1016/j.amc.2010.02.002-
dcterms.abstractA numerical method is presented for solving the Maxwell-Dirac systems. The Maxwell equations with particle and current densities as the source terms are discretized explicitly. To guarantee the particle conservation, the Dirac equations coupled electromagnetic potentials are discretized by the time-splitting method and implicit finite difference. These numerical schemes are conservative in particle density and have second-order accuracy in time and space. One-dimensional numerical results are given to validate the accuracy and the conservation and three-dimensional examples are presented to describe dynamical behaviors of the Maxwell-Dirac system with several external potentials.-
dcterms.bibliographicCitationApplied Mathematics and Computation, 2010, v. 216, no. 4, p. 1096-1108-
dcterms.isPartOfApplied mathematics and computation-
dcterms.issued2010-
dc.identifier.isiWOS:000276105200008-
dc.identifier.scopus2-s2.0-77949916155-
dc.identifier.eissn1873-5649-
dc.identifier.rosgroupidr49352-
dc.description.ros2009-2010 > Academic research: refereed > Publication in refereed journal-
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