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Fröhlich modes in porous III-V semiconductors

dc.contributor.authorSarua, A.en_US
dc.contributor.authorMonecke, J.en_US
dc.contributor.authorIrmer, G.en_US
dc.contributor.authorTiginyanu, I. M.en_US
dc.contributor.authorGärtner, G.en_US
dc.contributor.authorHartnagel, Hans L.en_US
dc.date.accessioned2006-12-19T18:56:50Z
dc.date.available2006-12-19T18:56:50Z
dc.date.issued2001-08-06en_US
dc.identifier.citationSarua, A; Monecke, J; Irmer, G; Tiginyanu, I M; Gärtner, G; Hartnagel, H L (2001). "Fröhlich modes in porous III-V semiconductors." Journal of Physics: Condensed Matter. 13(31): 6687-6706. <http://hdl.handle.net/2027.42/48888>en_US
dc.identifier.issn0953-8984en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/48888
dc.description.abstractPorous GaP, InP and GaAs structures fabricated by MeV ion-implantation-assisted electrochemical etching were investigated by Raman and Fourier transform infrared spectroscopy. Fröhlich modes in the frequency gap between the transverse optical and longitudinal optical frequencies were observed and their longitudinal-transverse splitting was established. The frequency-dependent optical properties in the infrared region were calculated using a dielectric function derived on the basis of an appropriate two-dimensional effective-medium theory. The theoretical reflectance spectra are found to be in good agreement with the experimental ones and the predicted coupled Fröhlich-plasmon modes for conducting samples were observed experimentally. The wavelength used in Raman measurements did not fulfil the requirements of effective-medium theory, but the resulting spectra could be explained at least qualitatively by taking into account the diffuse scattering.en_US
dc.format.extent3118 bytes
dc.format.extent616994 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.language.isoen_US
dc.publisherIOP Publishing Ltden_US
dc.titleFröhlich modes in porous III-V semiconductorsen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Electrical Engineering and Computer Science, The University of Michigan, 1301 Beal Avenue, Ann Arbor, MI 48109-2122, USA; Institute of Applied Physics, Technical University of Moldova, Boulevard Stefan cel Mare 168, MD-2004 Chisinau, Moldovaen_US
dc.contributor.affiliationotherInstitut für Theoretische Physik, TU Bergakademie Freiberg, Bernhard-von-Cotta-Strasse 4, D-09596 Freiberg, Germanyen_US
dc.contributor.affiliationotherInstitut für Theoretische Physik, TU Bergakademie Freiberg, Bernhard-von-Cotta-Strasse 4, D-09596 Freiberg, Germanyen_US
dc.contributor.affiliationotherInstitut für Theoretische Physik, TU Bergakademie Freiberg, Bernhard-von-Cotta-Strasse 4, D-09596 Freiberg, Germanyen_US
dc.contributor.affiliationotherInstitut für Experimentelle Physik, TU Bergakademie Freiberg, Silbermannstrasse 1, D-09596 Freiberg, Germanyen_US
dc.contributor.affiliationotherInstitut für Hochfrequenztechnik, TU Darmstadt, Merckstrasse 25, D-64283 Darmstadt, Germanyen_US
dc.contributor.affiliationumcampusAnn Arboren_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/48888/2/c13109.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1088/0953-8984/13/31/309en_US
dc.identifier.sourceJournal of Physics: Condensed Matter.en_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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