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Y. Makhlin, Gerd Schon, and Alexander Shnirman, Phys. Rev. Lett. 85, 4578 (2000);
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Makhlin, Y.1
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Y. MakhlinGerd SchonAlexander ShnirmanRev. Mod. Phys. 73, 357 (2001).
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Rev. Mod. Phys.
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Makhlin, Y.1
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4
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85038332550
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quant-ph/0008114 (unpublished);
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D.V. Averin, quant-ph/0008114 (unpublished);
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Averin, D.V.1
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5
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85038324864
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cond-mat/0004364 (unpublished)
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D.V. Averincond-mat/0004364 (unpublished).
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Averin, D.V.1
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7
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85038313322
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V.B. Braginsky and F.Y. Khalili, Quantum Measurement (Cambridge University Press, Cambridge, 1992)
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V.B. Braginsky and F.Y. Khalili, Quantum Measurement (Cambridge University Press, Cambridge, 1992).
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9
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0001082142
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Pis’ma Zh. Eksp. Teor. Fiz. 48, 218 (1988)
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L.I. Glazman, G.B. Lesovik, D.E. Khmelnitskii, and R.I. Shekhter, Pis’ma Zh. Eksp. Teor. Fiz. 48, 218 (1988) [JETP Lett. 48, 238 (1988)].
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JETP Lett.
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Glazman, L.I.1
Lesovik, G.B.2
Khmelnitskii, D.E.3
Shekhter, R.I.4
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13
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85038304052
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Note that in Ref. 2, the quantum limit is written as χ<2. This results from using a definition of (Formula presented) that is twice as large as the one used here
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Note that in Ref. 2, the quantum limit is written as χ<2. This results from using a definition of (Formula presented) that is twice as large as the one used here.
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14
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85038272685
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The proportionality condition expressed in Eq. (16) only involves a subset of matrix elements, and is thus not incompatible with the operators (Formula presented) and (Formula presented) being Hermitian. In the case where the state (Formula presented) in this equation, one simply needs that the corresponding matrix elements of (Formula presented) and (Formula presented) vanish
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The proportionality condition expressed in Eq. (16) only involves a subset of matrix elements, and is thus not incompatible with the operators (Formula presented) and (Formula presented) being Hermitian. In the case where the state (Formula presented) in this equation, one simply needs that the corresponding matrix elements of (Formula presented) and (Formula presented) vanish.
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15
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85038285965
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E.C. Titchmarsh, Introduction to the Theory of Fourier Integrals (Oxford, University Press, Oxford, 1937)
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E.C. Titchmarsh, Introduction to the Theory of Fourier Integrals (Oxford, University Press, Oxford, 1937).
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16
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85038284996
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L.B. Levitin, in Quantum Communication and Measurement, edited by V.P. Belavkin, O. Hirota, and R.L. Hudson (Plenum Press, New York, 1995), p. 439
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L.B. Levitin, in Quantum Communication and Measurement, edited by V.P. Belavkin, O. Hirota, and R.L. Hudson (Plenum Press, New York, 1995), p. 439.
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17
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85038277260
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quant-ph/9601020 (unpublished);
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C.A. Fuchs, quant-ph/9601020 (unpublished);
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Fuchs, C.A.1
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20
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85174221129
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M.A. Nielsen and I.L. Chuang, Quantum Computation and Quantum Information (Cambridge University Press, Cambridge, 2000)
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M.A. Nielsen and I.L. Chuang, Quantum Computation and Quantum Information (Cambridge University Press, Cambridge, 2000).
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22
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85038336818
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More generally, there will be two different detector density matrices (Formula presented) corresponding to the two qubit states; we consider the case of pure states for simplicity
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More generally, there will be two different detector density matrices (Formula presented) corresponding to the two qubit states; we consider the case of pure states for simplicity.
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23
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84889281816
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See, e.g., T.M. Cover and J.A. Thomas, Elements of Information Theory (Wiley, New York, 1991)
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See, e.g., T.M. Cover and J.A. Thomas, Elements of Information Theory (Wiley, New York, 1991).
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24
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3042988056
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For simplicity, we do not consider self-consistency effects that can become important when the current is no longer linear with voltage, see, e.g., T. Christen and M. Büttiker, Europhys. Lett. 35, 523 (1996).
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(1996)
Europhys. Lett.
, vol.35
, pp. 523
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Christen, T.1
Büttiker, M.2
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0032568026
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E. Buks, R. Schuster, M. Heiblum, D. Mahalu, and V. Umansky, Nature (London) 391, 871 (1998).
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Nature (London)
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, pp. 871
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Buks, E.1
Schuster, R.2
Heiblum, M.3
Mahalu, D.4
Umansky, V.5
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26
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0033689317
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D. Sprinzak, E. Buks, M. Heiblum, and H. Shtrikman, Phys. Rev. Lett. 84, 5820 (2000).
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Phys. Rev. Lett.
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Sprinzak, D.1
Buks, E.2
Heiblum, M.3
Shtrikman, H.4
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27
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0004473015
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Ya.M. Blanter and M. Büttiker, Phys. Rep. 336, 1 (2000)
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Ya.M. Blanter and M. Büttiker, Phys. Rep. 336, 1 (2000).
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29
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85038285026
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Note that our Eq. (40) has a constant on the right-hand side, while the corresponding equation in Ref. 6 [Eq. (12)] has an arbitrary energy-dependent function on the right-hand side. This difference results from the fact that Ref. 6 considers voltages so small that the effects of energy averaging can be neglected
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Note that our Eq. (40) has a constant on the right-hand side, while the corresponding equation in Ref. 6 [Eq. (12)] has an arbitrary energy-dependent function on the right-hand side. This difference results from the fact that Ref. 6 considers voltages so small that the effects of energy averaging can be neglected.
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30
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85038334654
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Note that by left-right symmetry, we mean that the scalar potential (Formula presented) in the scattering region is a symmetric function of x, where x is the transport direction. One can still have an absence of time-reversal symmetry if, e.g., there is a vector potential in the scattering region
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Note that by left-right symmetry, we mean that the scalar potential (Formula presented) in the scattering region is a symmetric function of x, where x is the transport direction. One can still have an absence of time-reversal symmetry if, e.g., there is a vector potential in the scattering region.
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