Full metadata record
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Tsai, Jengjan | en_US |
dc.contributor.author | Chang, Cheng-Hung | en_US |
dc.date.accessioned | 2014-12-08T15:21:57Z | - |
dc.date.available | 2014-12-08T15:21:57Z | - |
dc.date.issued | 2012-02-22 | en_US |
dc.identifier.issn | 0953-8984 | en_US |
dc.identifier.uri | http://dx.doi.org/10.1088/0953-8984/24/7/075801 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/15625 | - |
dc.description.abstract | We 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.iso | en_US | en_US |
dc.title | Generalized path integral method for Elliott-Yafet spin relaxations in quantum wells and narrow wires | en_US |
dc.type | Article | en_US |
dc.identifier.doi | 10.1088/0953-8984/24/7/075801 | en_US |
dc.identifier.journal | JOURNAL OF PHYSICS-CONDENSED MATTER | en_US |
dc.citation.volume | 24 | en_US |
dc.citation.issue | 7 | en_US |
dc.citation.epage | en_US | |
dc.contributor.department | 物理研究所 | zh_TW |
dc.contributor.department | Institute of Physics | en_US |
dc.identifier.wosnumber | WOS:000300390500017 | - |
dc.citation.woscount | 0 | - |
Appears in Collections: | Articles |
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