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Volumn 64, Issue 3, 2001, Pages

Possibility of an electromechanical which-path interferometer

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE; CALCULATION; ELECTRIC FIELD; ELECTRON; INTERFEROMETER; MATHEMATICAL ANALYSIS; MECHANICS; PHYSICS; RADIOFREQUENCY;

EID: 0034905885     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.64.035311     Document Type: Article
Times cited : (37)

References (43)
  • 1
    • 0000307666 scopus 로고
    • P. A. Schilpp Library of Living Philosophers, Evanston, IL
    • N. Bohr, in Albert Einstein: Philosopher Scientist, edited by P. A. Schilpp (Library of Living Philosophers, Evanston, IL, 1949), Vol. 7, p. 200.
    • (1949) Albert Einstein: Philosopher Scientist , vol.7 , pp. 200
    • Bohr, N.1
  • 6
    • 0002906681 scopus 로고    scopus 로고
    • M. O. Scully, B.-G. Englert, and H. Walther, Nature (London) 351, 111 (1991)
    • M. O. Scully, B.-G. Englert, and H. Walther, Nature (London) 351, 111 (1991).
  • 9
    • 85038280839 scopus 로고    scopus 로고
    • cond-mat/0006361 (unpublished)
    • For a review of previous work on phase coherent transport and controlled dephasing see G. Hackenbroich, /cond-mat/0006361 (unpublished).
    • Hackenbroich, G.1
  • 23
    • 85038327368 scopus 로고    scopus 로고
    • Our assumption is that the which-path device is operated in a steady-state mode, whereby measurements are only made after any transitory behavior has decayed so that the probability distribution of (initial) cantilever states is stationary. This steady-state distribution is further assumed to be the usual thermal distribution. These assumptions will only be strictly correct in the limit as the current goes to zero, but can be expected to provide predictions which are at least qualitatively correct for the average behavior over long times even with finite currents
    • Our assumption is that the which-path device is operated in a steady-state mode, whereby measurements are only made after any transitory behavior has decayed so that the probability distribution of (initial) cantilever states is stationary. This steady-state distribution is further assumed to be the usual thermal distribution. These assumptions will only be strictly correct in the limit as the current goes to zero, but can be expected to provide predictions which are at least qualitatively correct for the average behavior over long times even with finite currents.
  • 25
    • 85038336425 scopus 로고    scopus 로고
    • We assume that all positions are measured from the equilibrium height of the cantilever above the dot, including the effect of the residual electrons on the dot which do not participate in the transport
    • We assume that all positions are measured from the equilibrium height of the cantilever above the dot, including the effect of the residual electrons on the dot which do not participate in the transport.
  • 27
    • 0012603633 scopus 로고
    • Zh. Éksp. Teor. Fiz. 94, 292 (1987)
    • L. I. Glazman and R. I. Shekhter, Zh. Éksp. Teor. Fiz. 94, 292 (1987) [Sov. Phys. JETP 67, 163 (1988)].
    • (1988) Sov. Phys. JETP , vol.67 , pp. 163
    • Glazman, L.I.1    Shekhter, R.I.2
  • 28
    • 0001013107 scopus 로고    scopus 로고
    • A.-P. Jauho and N. S. Wingreen, Phys. Rev. B 58, 9619 (1998)
    • A.-P. Jauho and N. S. Wingreen, Phys. Rev. B 58, 9619 (1998).
  • 36
    • 85038269803 scopus 로고    scopus 로고
    • (private communication)
    • E. Buks (private communication).
    • Buks, E.1
  • 42
    • 34347209835 scopus 로고    scopus 로고
    • H.-J. Butt and M. Jashchke, Nanotechnology 6, 1 (1995)
    • H.-J. Butt and M. Jashchke, Nanotechnology 6, 1 (1995).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.