-
2
-
-
33744608791
-
-
A. Schmid, Z. Phys. 271, 251 (1974).
-
(1974)
Z. Phys.
, vol.271
, pp. 251
-
-
Schmid, A.1
-
4
-
-
0343239894
-
-
H. Pothier, S. Guéron, Norman O. Birge, D. Esteve, and M. H. Devoret, Z. Phys. B 104, 178 (1997); Phys. Rev. Lett. 79, 3490 (1997).
-
(1997)
Z. Phys. B
, vol.104
, pp. 178
-
-
Pothier, H.1
Guéron, S.2
Birge, N.O.3
Esteve, D.4
Devoret, M.H.5
-
5
-
-
0000264032
-
-
H. Pothier, S. Guéron, Norman O. Birge, D. Esteve, and M. H. Devoret, Z. Phys. B 104, 178 (1997); Phys. Rev. Lett. 79, 3490 (1997).
-
(1997)
Phys. Rev. Lett.
, vol.79
, pp. 3490
-
-
-
9
-
-
0024011864
-
-
R. Landauer, IBM J. Res. Develop. 1, 223 (1957); 32, 306 (1988).
-
(1988)
IBM J. Res. Develop.
, vol.32
, pp. 306
-
-
-
10
-
-
0040389817
-
-
In all the experiments we have performed (on copper, gold and silver wires), the sheet resistance of the aluminum probe was of the order of 1 Ω. The superconducting finger was therefore far from the transition to an insulator, which makes the interpretation of our results in copper presented by B.N. Narozhny, I.L. Aleiner and B.L. Altshuler in Phys. Rev. B 60, 7213 (1999) doubtful. Moreover, the stronger rounding of the distribution functions measured in longer wires, which was systematically observed in experiments, is in strong contradiction with the conclusions of this model.
-
(1999)
Phys. Rev. B
, vol.60
, pp. 7213
-
-
Narozhny, B.N.1
Aleiner, I.L.2
Altshuler, B.L.3
-
11
-
-
36449006418
-
-
D. Vion, P.F. Orfila, P. Joyez, D. Esteve, and M. H. Devoret, J. Appl. Phys. 77, 2519 (1995).
-
(1995)
J. Appl. Phys.
, vol.77
, pp. 2519
-
-
Vion, D.1
Orfila, P.F.2
Joyez, P.3
Esteve, D.4
Devoret, M.H.5
-
12
-
-
0041945166
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-
note
-
The best fit was obtained with a reservoir temperature of 80 mK.
-
-
-
-
13
-
-
30244453170
-
-
K.E. Nagaev, Phys. Lett. A 169, 103 (1992); Phys. Rev. B 52, 4740 (1995).
-
(1992)
Phys. Lett. A
, vol.169
, pp. 103
-
-
Nagaev, K.E.1
-
14
-
-
0001043946
-
-
K.E. Nagaev, Phys. Lett. A 169, 103 (1992); Phys. Rev. B 52, 4740 (1995).
-
(1995)
Phys. Rev. B
, vol.52
, pp. 4740
-
-
-
15
-
-
85085718304
-
-
note
-
-1.
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-
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17
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0345504803
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We have used here a numerical prefactor which was deduced (along the lines of the Appendix in Ref. 17) from the corrected expression of the phase coherence time τφ given in: I.L. Aleiner, B.L. Altshuler, and M.E. Gershenson, Waves Random Media 9, 201 (1999). This prefactor is larger by a factor π√2 than the one deduced from the expression of the lifetime in Eq. (4.4) of Ref. 3.
-
(1999)
Waves Random Media
, vol.9
, pp. 201
-
-
Aleiner, I.L.1
Altshuler, B.L.2
Gershenson, M.E.3
-
19
-
-
0000676596
-
-
A. Zawadowski, Jan von Delft, D. C. Ralph, Phys. Rev. Lett. 83, 2632 (1999); Johann Kroha and A. Zawadowski, private communication.
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 2632
-
-
Zawadowski, A.1
Von Delft, J.2
Ralph, D.C.3
-
20
-
-
0000676596
-
-
private communication
-
A. Zawadowski, Jan von Delft, D. C. Ralph, Phys. Rev. Lett. 83, 2632 (1999); Johann Kroha and A. Zawadowski, private communication.
-
-
-
Kroha, J.1
Zawadowski, A.2
-
21
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0042445909
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this volume
-
A.B. Gougam, F. Pierre, H. Pothier, D. Esteve, and N.O. Birge, this volume.
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Gougam, A.B.1
Pierre, F.2
Pothier, H.3
Esteve, D.4
Birge, N.O.5
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