Please use this identifier to cite or link to this item: https://hdl.handle.net/10356/83530
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dc.contributor.authorBroer, Wijnanden
dc.contributor.authorLiow, John Yuh Hanen
dc.contributor.authorLu, Bing-Suien
dc.date.accessioned2019-08-23T07:43:58Zen
dc.date.accessioned2019-12-06T15:24:57Z-
dc.date.available2019-08-23T07:43:58Zen
dc.date.available2019-12-06T15:24:57Z-
dc.date.issued2019en
dc.identifier.citationBroer, W., Liow, J. Y. H., & Lu, B.-S. (2019). Maxwell eigenmode approach to the Casimir-Lifshitz torque. Physical Review A, 100(1), 012514-. doi:10.1103/PhysRevA.100.012514en
dc.identifier.issn2469-9926en
dc.identifier.urihttps://hdl.handle.net/10356/83530-
dc.description.abstractMore than 40 years ago, Barash published a calculation of the full retarded Casimir-Lifshitz torque for planar birefringent media with arbitrary degrees of anisotropy. An independent theoretical confirmation has been lacking since. We report a systematic and transparent derivation of the torque between two media with both electric and magnetic birefringence. Our approach, based on an eigenmode decomposition of Maxwell's equations, generalizes Barash's result for electrically birefringent materials, and can be generalized to a wide range of anisotropic materials and finite thickness effects.en
dc.format.extent15 p.en
dc.language.isoenen
dc.relation.ispartofseriesPhysical Review Aen
dc.rights© 2019 American Physical Society. All rights reserved. This paper was published in Physical Review A and is made available with permission of American Physical Societyen
dc.subjectMaxwellen
dc.subjectCasimiren
dc.subjectScience::Physicsen
dc.titleMaxwell eigenmode approach to the Casimir-Lifshitz torqueen
dc.typeJournal Articleen
dc.contributor.schoolSchool of Physical and Mathematical Sciencesen
dc.identifier.doi10.1103/PhysRevA.100.012514en
dc.description.versionPublished versionen
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