dc.contributor.author |
Anastassakis, E |
en |
dc.date.accessioned |
2014-03-01T01:13:19Z |
|
dc.date.available |
2014-03-01T01:13:19Z |
|
dc.date.issued |
1997 |
en |
dc.identifier.issn |
0021-8979 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/12432 |
|
dc.relation.uri |
http://www.scopus.com/inward/record.url?eid=2-s2.0-0008424644&partnerID=40&md5=cd8a347ded4e19216870eb43fdfa131e |
en |
dc.subject.classification |
Physics, Applied |
en |
dc.subject.other |
ANGULAR-DISPERSION |
en |
dc.subject.other |
HETEROSTRUCTURES |
en |
dc.subject.other |
SPECTROSCOPY |
en |
dc.title |
Selection rules of Raman scattering by optical phonons in strained cubic crystals |
en |
heal.type |
journalArticle |
en |
heal.language |
English |
en |
heal.publicationDate |
1997 |
en |
heal.abstract |
Strain characterization of materials through Raman spectroscopy often requires the optical phonon wave vector to be in directions other than those of the strain-modified phonon eigenvectors. As a result, the observed mode frequencies are mixtures of the strain-modified eigenfrequencies. The selection rules for such generalized scattering configurations are derived here for the strained zincblende-diamond family crystals. The formulation is based on the relative magnitude of the LO-TO and the strain-induced splittings. The results are important for the analysis of strain-modified Raman lineshapes and of ''forbidden'' lines. Specific examples;are worked out in derail for externally stressed bulk crystals (90 degrees scattering geometry), and for [001], [111], and [110] strained heterojunctions (backscattering under oblique incidence and/or detection). (C) 1997 American Institute of Physics. |
en |
heal.publisher |
AMER INST PHYSICS |
en |
heal.journalName |
Journal of Applied Physics |
en |
dc.identifier.isi |
ISI:A1997XQ79700012 |
en |
dc.identifier.volume |
82 |
en |
dc.identifier.issue |
4 |
en |
dc.identifier.spage |
1582 |
en |
dc.identifier.epage |
1591 |
en |