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dc.contributor.authorTsai, Jengjanen_US
dc.contributor.authorChang, Cheng-Hungen_US
dc.date.accessioned2014-12-08T15:21:57Z-
dc.date.available2014-12-08T15:21:57Z-
dc.date.issued2012-02-22en_US
dc.identifier.issn0953-8984en_US
dc.identifier.urihttp://dx.doi.org/10.1088/0953-8984/24/7/075801en_US
dc.identifier.urihttp://hdl.handle.net/11536/15625-
dc.description.abstractWe generalized the semiclassical path integral method originally used in the D'yakonov-Perel' mechanism to study the spin relaxation of the Elliott-Yafet mechanism in low-dimensional systems. In quantum wells, the spin properties calculated by this method confirmed the experimental results. In two-dimensional narrow wires, size and impurity effects on the Elliott-Yafet relaxation were predicted, including the wire-width-dependent relaxation time, the polarization evolution on the sample boundaries, and the relaxation behavior during the diffusive-ballistic transition. These properties were compared with those of the D'yakonov-Perel' relaxation calculated under similar conditions. For ballistic narrow wires, we derived an exact relation between the Elliott-Yafet relaxation time and the wire width, which confirmed the above simulations.en_US
dc.language.isoen_USen_US
dc.titleGeneralized path integral method for Elliott-Yafet spin relaxations in quantum wells and narrow wiresen_US
dc.typeArticleen_US
dc.identifier.doi10.1088/0953-8984/24/7/075801en_US
dc.identifier.journalJOURNAL OF PHYSICS-CONDENSED MATTERen_US
dc.citation.volume24en_US
dc.citation.issue7en_US
dc.citation.epageen_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000300390500017-
dc.citation.woscount0-
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