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M. Switkes, C. M. Marcus, K. Campman, and A. C. Gossard, Science 283, 1905 (1999).
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0034667036
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J. E. Avron, A. Elgart, G. M. Graf, and L. Sadun, Phys. Rev. B 62, 10 618 (2000).
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Phys. Rev. B
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Avron, J.E.1
Elgart, A.2
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84902540342
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J. E. Avron, A. Elgart, G. M. Graf, and L. Sadun, Phys. Rev. Lett. 87, 236601 (2001);
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Avron, J.E.1
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J. E. AvronA. ElgartG. M. GrafL. SadunJ. Math. Phys. 43, 3415 (2002).
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Avron, J.E.1
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16
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85038285381
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unpublished
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A. Alekseev, (unpublished).
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Alekseev, A.1
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28
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85038291961
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unpublished
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S. W. Kim, (unpublished).
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Kim, S.W.1
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29
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85038333677
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unpublished
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D. Cohen, (unpublished).
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Cohen, D.1
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30
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85038332447
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The crossover from adiabatic to nonadiabatic transmission through a tunnel barrier with an additional small-amplitude oscillating potential was used in Ref. 29 to find the traversal time for tunneling. This yields a time scale that differs from the more widely used Wigner and Wigner-Smith times. We refer the interested reader to Ref. 30
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The crossover from adiabatic to nonadiabatic transmission through a tunnel barrier with an additional small-amplitude oscillating potential was used in Ref. 29 to find the traversal time for tunneling. This yields a time scale that differs from the more widely used Wigner and Wigner-Smith times. We refer the interested reader to Ref. 30.
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32
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85038337970
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Time in Quantum Mechanics, edited by J. G. Muga, R. Sala Mayato and I. L. Egusquiza, Springer-Verlag, Berlin
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Time in Quantum Mechanics, edited by J. G. Muga, R. Sala Mayato and I. L. Egusquiza (Springer-Verlag, Berlin, 2002).
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45
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22444452374
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M. V. Moskalets, Zh. Éksp. Teor. Fiz. 114, 1827 (1998) [JETP 87, 991 (1998)].
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Moskalets, M.V.1
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47
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85038267744
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The same problem but with a single oscillating (formula presented)-function barrier was considered in Ref. 36
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The same problem but with a single oscillating (formula presented)-function barrier was considered in Ref. 36.
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48
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0034664451
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The phase change by (formula presented) in consecutive resonances is special for the two-barrier model considered here. For systems with lateral extent the phase change of consecutive resonances is randomly (formula presented) or (formula presented) [see
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The phase change by (formula presented) in consecutive resonances is special for the two-barrier model considered here. For systems with lateral extent the phase change of consecutive resonances is randomly (formula presented) or (formula presented) [see A. Levy Yeyati and M. Büttiker, Phys. Rev. B 62, 7307 (2000)].
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Phys. Rev. B
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Levy Yeyati, A.1
Büttiker, M.2
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49
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85038298994
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Note that the phase coherent pump effect discussed here should be distinguished from the rectification of displacement currents recently discussed by Brouwer (Ref. 9) and Polianski and Brouwer (Ref. 10), which is closely related to the setup of the experiment of Switkes et al. (Ref. 1) and should be distinguished from the rectification due to inelastic scattering discussed in Ref. 11
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Note that the phase coherent pump effect discussed here should be distinguished from the rectification of displacement currents recently discussed by Brouwer (Ref. 9) and Polianski and Brouwer (Ref. 10), which is closely related to the setup of the experiment of Switkes et al. (Ref. 1) and should be distinguished from the rectification due to inelastic scattering discussed in Ref. 11.
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50
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3343004181
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The phase of a quantum dot cannot be determined in a two-terminal conductance measurement [see
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The phase of a quantum dot cannot be determined in a two-terminal conductance measurement [see A. Yacoby, M. Heiblum, D. Mahalu, and H. Shtrikman, Phys. Rev. Lett. 74, 4047 (1995)] but requires multiterminal measurements
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Yacoby, A.1
Heiblum, M.2
Mahalu, D.3
Shtrikman, H.4
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52
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0000799054
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for an early discussion and for a broader review
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for an early discussion and for a broader review, G. Hackenbroich, Phys. Rep. 343, 464 (2001)]. In contrast nonadiabatic pumping proposed here permits a two-terminal geometry.
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(2001)
Phys. Rep.
, vol.343
, pp. 464
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Hackenbroich, G.1
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