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Volumn 64, Issue 15, 2001, Pages

Thermal transport through a mesoscopic weak link

Author keywords

[No Author keywords available]

Indexed keywords

SILICON;

EID: 0006235902     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.64.155320     Document Type: Article
Times cited : (58)

References (24)
  • 6
    • 0003957805 scopus 로고
    • M. Reed, Academic Press, San Diego, in, edited by, 35
    • M. Büttiker, in Semiconductors and Semimetals, edited by M. Reed (Academic Press, San Diego, 1992), Vol. 35.
    • (1992) Semiconductors and Semimetals
    • Büttiker, M.1
  • 7
    • 85038916080 scopus 로고    scopus 로고
    • The Landauer formula can be applied to the case of weak tunneling provided one includes an energy-dependent transmission probability for each channel. However, these transmission probabilities have to be calculated microscopically, which, in the weak-tunneling limit, amounts to using our approach
    • The Landauer formula can be applied to the case of weak tunneling provided one includes an energy-dependent transmission probability for each channel. However, these transmission probabilities have to be calculated microscopically, which, in the weak-tunneling limit, amounts to using our approach.
  • 9
    • 85038958856 scopus 로고    scopus 로고
    • See also G. D. Mahan, 3rd ed. (Plenum, New York, 2000)
    • See also G. D. Mahan, Many-Particle Physics, 3rd ed. (Plenum, New York, 2000).
  • 19
    • 85038916437 scopus 로고    scopus 로고
    • Note that (formula presented)
    • Note that (formula presented).
  • 21
    • 85038942326 scopus 로고    scopus 로고
    • This is correct only at the low energies of interest in the present work. At higher energies it is of course possible to have forbidden regions, for example, in a vibrational band-gap structure, or simply at energies higher than the acoustic and optical phonon bands of an ordinary crystal
    • This is correct only at the low energies of interest in the present work. At higher energies it is of course possible to have forbidden regions, for example, in a vibrational band-gap structure, or simply at energies higher than the acoustic and optical phonon bands of an ordinary crystal.
  • 23
    • 85038897970 scopus 로고    scopus 로고
    • Here ‘(formula presented)’ denotes the Rayleigh branch
    • Here ‘(formula presented)’ denotes the Rayleigh branch.
  • 24
    • 85038937993 scopus 로고    scopus 로고
    • It is useful to compare this result to the corresponding, spectral density of an isotropic elastic continuum, calculated with periodic boundary conditions, (formula presented)
    • It is useful to compare this result to the corresponding bulk spectral density of an isotropic elastic continuum, calculated with periodic boundary conditions, (formula presented)


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.