000111029 001__ 111029
000111029 005__ 20181203020924.0
000111029 0247_ $$2doi$$a10.1103/PhysRevB.58.R10175
000111029 022__ $$a0163-1829
000111029 037__ $$aARTICLE
000111029 245__ $$aResonant Rayleigh scattering versus incoherent luminescence in semiconductor microcavities
000111029 260__ $$c1998
000111029 269__ $$a1998
000111029 336__ $$aJournal Articles
000111029 500__ $$aSwiss Fed Inst Technol, Dept Phys, Inst Micro & Optoelect, CH-1015 Lausanne, Switzerland. Hitachi Cambridge Lab, Cambridge CB3 0HE, England. Swiss Fed Inst Technol, Dept Phys, Inst Micro & Optoelect, CH-1015 Lausanne, Switzerland. Hayes, GR, Swiss Fed Inst Technol, Dept Phys, Inst Micro & Optoelect, CH-1015 Lausanne, Switzerland.
000111029 500__ $$aISI Document Delivery No.: 133ZB
000111029 500__ $$aTimes Cited: 0
000111029 500__ $$aCited Reference Count: 13
000111029 500__ $$aCited References: 
000111029 500__ $$a     BONGIOVANNI G, 1997, PHYS REV B, V55, P7084
000111029 500__ $$a     CITRIN DS, 1996, PHYS REV B, V54, P14572
000111029 500__ $$a     GURIOLI M, 1997, PHYS REV LETT, V78, P3205
000111029 500__ $$a     HAACKE S, 1997, PHYS REV LETT, V78, P2228
000111029 500__ $$a     HAACKE S, 1998, J OPT SOC AM B, V15, P1410
000111029 500__ $$a     HEBERLE AP, 1994, PHYS REV LETT, V72, P3887
000111029 500__ $$a     HOUDRE R, 1994, PHYS REV LETT, V73, P2043
000111029 500__ $$a     NORRIS TB, 1994, PHYS REV B, V50, P14663
000111029 500__ $$a     STOLZ H, 1993, PHYS REV B, V47, P9669
000111029 500__ $$a     VINATTIERI A, 1994, PHYS REV B, V50, P10868
000111029 500__ $$a     WANG HL, 1995, PHYS REV LETT, V74, P3065
000111029 500__ $$a     WEISBUCH C, 1992, PHYS REV LETT, V69, P3314
000111029 500__ $$a     ZIMMERMANN R, 1995, NUOVO CIMENTO D, V17, P1801
000111029 520__ $$aIt is demonstrated that during the first few picoseconds after resonant femtosecond excitation the secondary radiation from a strongly coupled semiconductor microcavity containing one quantum well is dominated by Rayleigh scattered light. At early times after excitation (<10 ps) the two polariton modes emit with almost equal intensity resulting in a strong beating of the emission. For longer times (>10 ps) the lower polariton branch provides the most intense emission which is due to incoherent luminescence. The results in the Ray leigh scattering regime are shown to be in excellent agreement with a theoretical model of coherence transfer due to interface roughness. [S0163-1829(98)52940-2].
000111029 6531_ $$aGAAS QUANTUM-WELLS
000111029 6531_ $$aEXCITONS
000111029 6531_ $$aEMISSION
000111029 6531_ $$aEXCITATION
000111029 6531_ $$aCOHERENT
000111029 6531_ $$aDYNAMICS
000111029 700__ $$0241671$$aHayes, G. R.$$g111189
000111029 700__ $$0241798$$aHaacke, S.$$g105346
000111029 700__ $$aKauer, M.
000111029 700__ $$aStanley, R. P.
000111029 700__ $$0240344$$aHoudre, R.$$g105419
000111029 700__ $$0241200$$aOesterle, U.$$g107464
000111029 700__ $$0241178$$aDeveaud, B.$$g104954
000111029 773__ $$j58$$k16$$qR10175-R10178$$tPhysical Review B
000111029 909C0 $$0252003$$pLOEQ$$xU10156
000111029 909C0 $$0253378$$pSCI-SB-RH$$xU13466
000111029 909CO $$ooai:infoscience.tind.io:111029$$pSB$$particle
000111029 937__ $$aLOEQ-ARTICLE-1998-023
000111029 970__ $$a107/LOEQ
000111029 973__ $$aEPFL$$rREVIEWED$$sPUBLISHED
000111029 980__ $$aARTICLE