-
4
-
-
22844455536
-
-
JUPSAU 0031-9015 10.1143/JPSJ.68.2172
-
S. Misawa, J. Phys. Soc. Jpn. JUPSAU 0031-9015 10.1143/JPSJ.68.2172 68, 2172 (1999).
-
(1999)
J. Phys. Soc. Jpn.
, vol.68
, pp. 2172
-
-
Misawa, S.1
-
5
-
-
17644437092
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.86.5337
-
G. Y. Chitov and A. J. Millis, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.86.5337 86, 5337 (2001);
-
(2001)
Phys. Rev. Lett.
, vol.86
, pp. 5337
-
-
Chitov, G.Y.1
Millis, A.J.2
-
6
-
-
0035425389
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.64.054414
-
G. Y. Chitov and A. J. Millis, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.64.054414 64, 054414 (2001).
-
(2001)
Phys. Rev. B
, vol.64
, pp. 054414
-
-
Chitov, G.Y.1
Millis, A.J.2
-
7
-
-
2542484981
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.68.155113
-
A. V. Chubukov and D. L. Maslov, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.68.155113 68, 155113 (2003);
-
(2003)
Phys. Rev. B
, vol.68
, pp. 155113
-
-
Chubukov, A.V.1
Maslov, D.L.2
-
8
-
-
2342439768
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.69.121102
-
A. V. Chubukov and D. L. Maslov, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.69.121102 69, 121102 (R) (2004).
-
(2004)
Phys. Rev. B
, vol.69
, pp. 121102
-
-
Chubukov, A.V.1
Maslov, D.L.2
-
10
-
-
27144489376
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.95.026402
-
A. V. Chubukov, D. L. Maslov, S. Gangadharaiah, and L. I. Glazman, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.95.026402 95, 026402 (2005).
-
(2005)
Phys. Rev. Lett.
, vol.95
, pp. 026402
-
-
Chubukov, A.V.1
Maslov, D.L.2
Gangadharaiah, S.3
Glazman, L.I.4
-
11
-
-
29744435869
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.72.115112
-
J. Betouras, D. Efremov, and A. Chubukov, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.72.115112 72, 115112 (2005).
-
(2005)
Phys. Rev. B
, vol.72
, pp. 115112
-
-
Betouras, J.1
Efremov, D.2
Chubukov, A.3
-
12
-
-
0038502191
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.67.205407
-
O. Prus, Y. Yaish, M. Reznikov, U. Sivan, and V. Pudalov, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.67.205407 67, 205407 (2003).
-
(2003)
Phys. Rev. B
, vol.67
, pp. 205407
-
-
Prus, O.1
Yaish, Y.2
Reznikov, M.3
Sivan, U.4
Pudalov, V.5
-
13
-
-
4244094906
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.44.1469
-
F. Stern, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.44.1469 44, 1469 (1980).
-
(1980)
Phys. Rev. Lett.
, vol.44
, pp. 1469
-
-
Stern, F.1
-
14
-
-
21544442115
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.33.1076
-
A. Gold and V. T. Dolgopolov, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.33.1076 33, 1076 (1986).
-
(1986)
Phys. Rev. B
, vol.33
, pp. 1076
-
-
Gold, A.1
Dolgopolov, V.T.2
-
15
-
-
0000444781
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.33.5401
-
S. Das Sarma, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.33.5401 33, 5401 (1986).
-
(1986)
Phys. Rev. B
, vol.33
, pp. 5401
-
-
Das Sarma, S.1
-
16
-
-
33845271531
-
-
For the amplitude Γ(π) there is also a possibility to look on it in the zero-sound channel. Here a delicate question arises whether a singular combination vF k/(ω- vF k) typical for the particle-hole channel (Ref.) is of any importance. The calculation in Appendix shows that the anomalous part in the product of four Green's functions accumulates from vF k∼ vF p ω. Therefore, when it is treated in the Cooper channel, the bare value for the amplitude Γ(π) is the static amplitude Γk in the particle-hole channel.
-
For the amplitude Γ(π) there is also a possibility to look on it in the zero-sound channel. Here a delicate question arises whether a singular combination vF k/(ω- vF k) typical for the particle-hole channel (Ref.) is of any importance. The calculation in Appendix shows that the anomalous part in the product of four Green's functions accumulates from vF k∼ vF p ω. Therefore, when it is treated in the Cooper channel, the bare value for the amplitude Γ(π) is the static amplitude Γk in the particle-hole channel.
-
-
-
-
17
-
-
0038707782
-
-
E. M. Lifshitz and L. P. Pitaevskii, Statistical Physics, Part 2 Pergamon Press, Oxford
-
L. D. Landau and E. M. Lifshitz, Course of Theoretical Physics, Vol. 9, E. M. Lifshitz and L. P. Pitaevskii, Statistical Physics, Part 2 (Pergamon Press, Oxford, 1980).
-
(1980)
Course of Theoretical Physics
, vol.9
-
-
Landau, L.D.1
Lifshitz, E.M.2
-
18
-
-
33845260416
-
-
The nonanalytic terms are also generated by the rescattering of particle-hole pairs in the zero-sound channel. The overlap of all three channels leads to important consequences for the interpretation of the experimental data reported in Ref.. This is a subject of a separate publication. For more details see the end of Sec. 4.
-
The nonanalytic terms are also generated by the rescattering of particle-hole pairs in the zero-sound channel. The overlap of all three channels leads to important consequences for the interpretation of the experimental data reported in Ref.. This is a subject of a separate publication. For more details see the end of Sec. 4.
-
-
-
-
21
-
-
33750063925
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.74.165108
-
G. Schwiete, and K. B. Efetov, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.74.165108 74, 165108 (2006).
-
(2006)
Phys. Rev. B
, vol.74
, pp. 165108
-
-
Schwiete, G.1
Efetov, K.B.2
-
22
-
-
33746820575
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.74.075102
-
I. L. Aleiner and K. B. Efetov, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.74.075102 74, 075102 (2006).
-
(2006)
Phys. Rev. B
, vol.74
, pp. 075102
-
-
Aleiner, I.L.1
Efetov, K.B.2
-
23
-
-
0000345412
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.15.524
-
W. Kohn and J. M. Luttinger, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.15.524 15, 524 (1965);
-
(1965)
Phys. Rev. Lett.
, vol.15
, pp. 524
-
-
Kohn, W.1
Luttinger, J.M.2
-
24
-
-
0001620005
-
-
see also PRBMDO 0163-1829 10.1103/PhysRevB.48.1097
-
see also A. V. Chubukov, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.48.1097 48, 1097 (1993);
-
(1993)
Phys. Rev. B
, vol.48
, pp. 1097
-
-
Chubukov, A.V.1
-
25
-
-
0038778603
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.67.144520
-
V. M. Galitski and S. Das Sarma, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.67.144520 67, 144520 (2003).
-
(2003)
Phys. Rev. B
, vol.67
, pp. 144520
-
-
Galitski, V.M.1
Das Sarma, S.2
-
29
-
-
33845246234
-
-
It has been checked that these terms involve combinations of harmonics which do not reduce to the backward scattering amplitude. Unlike the two section term, there is only a weak logarithmic singularity near the backward scattering, which is not enough to make the logarithmic renormalizations important in channels other than the Cooper channel.
-
It has been checked that these terms involve combinations of harmonics which do not reduce to the backward scattering amplitude. Unlike the two section term, there is only a weak logarithmic singularity near the backward scattering, which is not enough to make the logarithmic renormalizations important in channels other than the Cooper channel.
-
-
-
|