-
11
-
-
16444377984
-
-
In the same spirit, but for the different problem of the fractional quantum Hall effect, see M. R. Geller, et al., Phys. Rev. Lett. 77, 4612 (1997).
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Phys. Rev. Lett.
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Geller, M.R.1
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14
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0000260497
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Phys. Rev. BV. V. Ponomarenko, 52, R8666 (1995).
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(1995)
, vol.52
, pp. R8666
-
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Ponomarenko, V.V.1
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15
-
-
0030527826
-
-
The result (Formula presented) was recovered without leads by A. Kawabata, J. Phys. Soc. Jpn. 65, 30 (1996);
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(1996)
J. Phys. Soc. Jpn.
, vol.65
, pp. 30
-
-
Kawabata, A.1
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17
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4243484397
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R. Egger and H. Grabert, Phys. Rev. Lett. 77, 538 (1996). But this requires the current to be not renormalized by the interactions (Ref. 12).
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(1996)
Phys. Rev. Lett.
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Egger, R.1
Grabert, H.2
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20
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0005065267
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-II)
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I. Safi, Phys. Rev. B 55, R7331 (1997-II).
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Phys. Rev. B
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Safi, I.1
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21
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85038286765
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-
I. Safi and H. J. Schulz, in Quantum Transport in Semiconductor Submicron Structures, edited by B. Kramer (Kluwer Academic Press, Dordrecht, 1995), Chap. 3, p. 159
-
I. Safi and H. J. Schulz, in Quantum Transport in Semiconductor Submicron Structures, edited by B. Kramer (Kluwer Academic Press, Dordrecht, 1995), Chap. 3, p. 159.
-
-
-
-
22
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-
33846983640
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-
) (the results hold only in the bulk of the wire)
-
D. L. Maslov, Phys. Rev. B 52, R14 368 (1995) (the results hold only in the bulk of the wire).
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(1995)
Phys. Rev. B
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Maslov, D.L.1
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24
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-
85038334270
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I. Safi, Ph.D. thesis, Laboratoire de Physique des Solides, Orsay (1996)
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I. Safi, Ph.D. thesis, Laboratoire de Physique des Solides, Orsay (1996);
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-
-
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25
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85033111911
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-
Ann. Phys. (Paris) 22, 463(1997).
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(1997)
Ann. Phys. (Paris)
, vol.22
, pp. 463
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-
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27
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85038326748
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-
Phys. Rev. BX. G. Wen43, 11 025 (1991).
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(1991)
, vol.43
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Wen, X.G.1
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32
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0000433883
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A. F. Andreev, Zh. Éksp. Teor. Fiz. 46, 1823 (1964) [Sov. Phys. JETP 19, 1228 (1964)].
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Sov. Phys. JETP
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Andreev, A.F.1
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36
-
-
4243537729
-
-
where the fluctuations of the conductance are computed in the infinite wire for spinless electrons, and coincide with our results only in the high-temperature limit and for spinless electrons
-
After the original version of this paper was submitted, there appeared a paper by Scot R. Renn and Daniel P. Arovas, Phys. Rev. Lett. 78, 4091 (1997)where the fluctuations of the conductance are computed in the infinite wire for spinless electrons, and coincide with our results only in the high-temperature limit and for spinless electrons.
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Phys. Rev. Lett.
, vol.78
, pp. 4091
-
-
-
39
-
-
85038337437
-
-
We subtract a formally infinite constant from (Formula presented). As all results depend only on differences of (Formula presented)’s, this is of no importance
-
We subtract a formally infinite constant from (Formula presented). As all results depend only on differences of (Formula presented)’s, this is of no importance.
-
-
-
-
40
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-
0004266550
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-
Elsevier, Amsterdam J. Zinn-Justin J. L. Pichard G. Montambaux E. Akkermans
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C. W. Beenakker, in Mesoscopic Quantum Physics, Les Houches Summer School Course No. LXI, edited by E. Akkermans, G. Montambaux, J. L. Pichard, and J. Zinn-Justin (Elsevier, Amsterdam, 1995).
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Mesoscopic Quantum Physics, Les Houches Summer School Course No. LXI
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Beenakker, C.W.1
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42
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-
0542426536
-
-
), where the local density of states is computed
-
In these previous works, we have studied the pairing correlation functions. See also a recent paper by D. L. Maslov and P. Goldbart, Phys. Rev. B 57, 9879 (1998), where the local density of states is computed.
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(1998)
Phys. Rev. B
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Maslov, D.L.1
Goldbart, P.2
-
46
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-
85038327742
-
-
We have to point out that our discussion is different from that of Ref. 32 where the competition between (Formula presented) and (Formula presented) is investigated for electrons without spin, in a wire without leads
-
We have to point out that our discussion is different from that of Ref. 32 where the competition between (Formula presented) and (Formula presented) is investigated for electrons without spin, in a wire without leads.
-
-
-
-
47
-
-
85038268030
-
-
Strictly speaking, this is true only for (Formula presented). Otherwise, the function (Formula presented) has to be replaced by a higher-order term that emanates from the integration of Eq. (3.13)
-
Strictly speaking, this is true only for (Formula presented). Otherwise, the function (Formula presented) has to be replaced by a higher-order term that emanates from the integration of Eq. (3.13).
-
-
-
-
49
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-
0000671436
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-
A possible explanation based on external effects was proposed recently by A. Yu. Alekseev and V. Cheianov, Phys. Rev. B 57, R6834 (1998).
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(1998)
Phys. Rev. B
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, pp. R6834
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Yu. Alekseev, A.1
Cheianov, V.2
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51
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0003498504
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-
Academic Press, London
-
I. S. Gradshteyn and I. M. Ryzhik, Table of Integrals, Series, and Products (Academic Press, London, 1980), formula 9.180.1.
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(1980)
Table of Integrals, Series, and Products
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-
Gradshteyn, I.S.1
Ryzhik, I.M.2
-
52
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85038345195
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-
Inès Safi (unpublished)
-
Inès Safi (unpublished).
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