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Volumn 53, Issue 11, 1996, Pages 6889-6892

Electron-electron scattering in far-infrared quantum cascade lasers

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EID: 0000877696     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.53.6889     Document Type: Article
Times cited : (46)

References (15)
  • 6
    • 0029634129 scopus 로고
    • The experimentally investigated isolated quantum-well sample constitutes the central region of our hypothetical far-infrared tunneling structure; see Fig. 1
    • J. N. Heyman, K. Unterrainer, K. Craig, B. Galdrikian, M. S. Sherwin, K. Campman, P. F. Hopkins and A. C. Gossard, Phys. Rev. Lett. 74, 2682 (1995). The experimentally investigated isolated quantum-well sample constitutes the central region of our hypothetical far-infrared tunneling structure; see Fig. 1.
    • (1995) Phys. Rev. Lett. , vol.74 , pp. 2682
    • Heyman, J.1    Unterrainer, K.2    Craig, K.3    Galdrikian, B.4    Sherwin, M.5    Campman, K.6    Hopkins, P.7    Gossard, A.8
  • 10
    • 33744572650 scopus 로고
    • We estimate [see J. Bardeen, Phys. Rev. Lett. 6, 57 (1961) and N. S. Wingreen, Ph.D. dissertation, Cornell University, 1989] (Formula presented) ≈((Formula presented) /(Formula presented))(Formula presented) ((Formula presented)) with velocity (Formula presented)=(Formula presented), transmission probability (Formula presented)(E)=(Formula presented)texp[-(Formula presented)(Formula presented)]/((Formula presented)-E), lower collector band edge (Formula presented), and assuming a (Formula presented) =30 Å ((Formula presented) =214 meV) barrier thickness (height.) For the structure shown in Fig. 1 we predict only a (Formula presented) =0.40(0.93) meV to (Formula presented) =0.56(1.09) meV variation within the range 12≲V≲30 mV of voltage drops ensuring the upper-subband current injection. We neglect electron charging effects in these estimates of (Formula presented), noting that a (Formula presented) electron sheet density causes just a 10% change in the internal field ≈V/(Formula presented) at V∼20 mV. The moderate variation in (Formula presented) can be negated by a small change in the barrier thickness.
    • (1961) Phys. Rev. Lett. , vol.6 , pp. 57
    • Bardeen, J.1
  • 11
    • 0000029135 scopus 로고
    • The strong nonequilibrium electron-electron scattering may also affect the study [see, for example, A. N. Korotkov, D. V. Averin and K. K. Likharev, Phys. Rev. B 49, 7548 (1994)] of possible continuous Bloch oscillations in a two-level tunneling structure.
    • (1994) Phys. Rev. B , vol.49 , pp. 7548
    • Korotkov, A.1    Averin, D.2    Likharev, K.3
  • 14
  • 15
    • 12044254665 scopus 로고
    • this paper reports and explains the corresponding voltage-drop dependence of the optical selection rules
    • J. Faist, F. Capasso, A. L. Hutchinson, L. Pfeiffer and K. W. West, Phys. Rev. Lett. 71, 3573 (1993); this paper reports and explains the corresponding voltage-drop dependence of the optical selection rules.
    • (1993) Phys. Rev. Lett. , vol.71 , pp. 3573
    • Faist, J.1    Capasso, F.2    Hutchinson, A.3    Pfeiffer, L.4    West, K.5


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.