메뉴 건너뛰기




Volumn 59, Issue 4, 1999, Pages 2824-2832

Frequency-dependent magnetotransport and particle dynamics in magnetic modulation systems

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0001521351     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.59.2824     Document Type: Article
Times cited : (8)

References (25)
  • 1
    • 85037915270 scopus 로고    scopus 로고
    • and D. Weiss, ibid., p. 327. For reviews see: K. Ensslin and R. Schuster, in Quantum Dynamics of Submicron Structures, NATO ASI Vol. 291, edited by H.A. Cerdeira, B. Kramer, and G. Schön (Kluwer, Dordrecht, 1995), p. 247;
    • For reviews see: K. Ensslin and R. Schuster, in Quantum Dynamics of Submicron Structures, NATO ASI Vol. 291, edited by H.A. Cerdeira, B. Kramer, and G. Schön (Kluwer, Dordrecht, 1995), p. 247;and D. Weiss, ibid., p. 327.
  • 19
    • 85037921586 scopus 로고    scopus 로고
    • The introduction of (Formula presented) guarantees particle diffusion for long times, and suppresses the possible anomalous diffusion and concomitant divergence of (Formula presented) for low frequencies. See Wagenhuber et al., Ref. 4. We choose typical values for the scattering time of (Formula presented) sec (or (Formula presented) for a relatively good mobility in GaAs of 30 (Formula presented) although our conclusions are insensitive to the detailed value of (Formula presented) as we illustrate.
    • The introduction of (Formula presented) guarantees particle diffusion for long times, and suppresses the possible anomalous diffusion and concomitant divergence of (Formula presented) for low frequencies. See Wagenhuber et al., Ref. 4. We choose typical values for the scattering time of (Formula presented) sec (or (Formula presented) for a relatively good mobility in GaAs of 30 (Formula presented) although our conclusions are insensitive to the detailed value of (Formula presented) as we illustrate.
  • 22
    • 0003831091 scopus 로고
    • Pergamon, New York
    • Notice that since the modulation is magnetic, the particle does not really “collide” with maxima, as in the case of an electrostatic modulation. Here, the particle trajectory continually decreases its radius of curvature as it approaches a more intense field, and is then deflected away from it much more smoothly than in the electrostatic/scalar potential case. See, e.g., L.D. Landau and E.M. Lifshitz, The Classical Theory of Fields (Pergamon, New York, 1975).
    • (1975) The Classical Theory of Fields
    • Landau, L.D.1    Lifshitz, E.M.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.