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Volumn 97, Issue 1, 2010, Pages

Long exciton spin relaxation in coupled quantum wells

Author keywords

[No Author keywords available]

Indexed keywords

COUPLED QUANTUM WELL; COUPLED QUANTUM WELL STRUCTURE; DEGREE OF CIRCULAR POLARIZATION; EXCITON SPIN RELAXATION; EXCITON STATE; INDIRECT EXCITONS; INDIRECT TRANSITION; RADIATIVE LIFETIME; SPIN RELAXATION TIME; TIME-RESOLVED PHOTOLUMINESCENCE;

EID: 77954753825     PISSN: 00036951     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3458703     Document Type: Article
Times cited : (23)

References (22)
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    • D. W. Snoke, Photonics Spectra PHSAD3 0731-1230 40, 108 (2006).
    • (2006) Photonics Spectra , vol.40 , pp. 108
    • Snoke, D.W.1
  • 7
    • 0033579345 scopus 로고    scopus 로고
    • SCIEAS 0036-8075,. 10.1126/science.286.5448.2312
    • T. Lundstrom, W. Schoenfeld, H. Lee, and P. M. Petroff, Science SCIEAS 0036-8075 286, 2312 (1999). 10.1126/science.286.5448.2312
    • (1999) Science , vol.286 , pp. 2312
    • Lundstrom, T.1    Schoenfeld, W.2    Lee, H.3    Petroff, P.M.4
  • 15
    • 0000442854 scopus 로고
    • 0ab V (x) -E dx], where mq,b -the carrier effective masses in quantum well and barrier materials, aq,b -QW and barrier thicknesses, E -energy of the lowest level in QW, V -barrier height modified by the electric field. See also, e.g., APPLAB 0003-6951, () 10.1063/1.101615;, Phys. Rev. B PRBMDO 0163-1829 40, 3028 (1989). 10.1103/PhysRevB.40.3028
    • 0ab V (x) -E dx], where mq,b -the carrier effective masses in quantum well and barrier materials, aq,b -QW and barrier thicknesses, E -energy of the lowest level in QW, V -barrier height modified by the electric field. See also, e.g., M. G. W. Alexander, W. W. Rühle, R. Sauer, and W. T. Tsang, Appl. Phys. Lett. APPLAB 0003-6951 55, 885 (1989) 10.1063/1.101615; D. Y. Oberli, J. Shah, T. C. Damen, C. W. Tu, T. Y. Chang, D. A. B. Miller, J. E. Henry, R. F. Kopf, N. Sauer, and A. E. DiGiovanni, Phys. Rev. B PRBMDO 0163-1829 40, 3028 (1989). 10.1103/PhysRevB.40.3028
    • (1989) Appl. Phys. Lett. , vol.55 , pp. 885
    • Alexander, M.G.W.1    Rühle, W.W.2    Sauer, R.3    Tsang, W.T.4    Oberli, D.Y.5    Shah, J.6    Damen, T.C.7    Tu, C.W.8    Chang, T.Y.9    Miller, D.A.B.10    Henry, J.E.11    Kopf, R.F.12    Sauer, N.13    Digiovanni, A.E.14
  • 18
    • 77954748306 scopus 로고    scopus 로고
    • The generated laser pulses have rectangular shape with fall and rise times of ∼1 ns. The "zero" of the time scale is defined by the end of the laser pulse. Negative values correspond to the measurements taken under laser illumination. For the estimation of the decay time we take only experimental points recorded after the laser pulse.
    • The generated laser pulses have rectangular shape with fall and rise times of ∼1 ns. The "zero" of the time scale is defined by the end of the laser pulse. Negative values correspond to the measurements taken under laser illumination. For the estimation of the decay time we take only experimental points recorded after the laser pulse.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.