-
2
-
-
0001135683
-
-
edited by R. D. Parks (Marcel Dekker, Inc., New York)
-
c superconductors tunneling information on the frequency dependence of the gap was used to explore the electron-phonon pairing mechanism; see, e.g., W. L. McMillan and J. M. Rowell, Super-conductivity, edited by R. D. Parks (Marcel Dekker, Inc., New York, 1969), Vol. 1, p. 561.
-
(1969)
Super-conductivity
, vol.1
, pp. 561
-
-
McMillan, W.L.1
Rowell, J.M.2
-
3
-
-
0032298898
-
-
J. Voit, Eur. Phys. J. B 5, 505 (1998); E.H. L. Essler and A. M. Tsvelik, cond-mat/0205294.
-
(1998)
Eur. Phys. J. B
, vol.5
, pp. 505
-
-
Voit, J.1
-
4
-
-
0032298898
-
-
cond-mat/0205294
-
J. Voit, Eur. Phys. J. B 5, 505 (1998); E.H. L. Essler and A. M. Tsvelik, cond-mat/0205294.
-
-
-
Essler, E.H.L.1
Tsvelik, A.M.2
-
9
-
-
0001175552
-
-
C. J. Morningstar and M. Weinstein, Phys. Rev. D 54, 4131 (1996). For Hubbard models, see E. Altman and A. Auerbach, Phys. Rev. B 65, 104508 (2002).
-
(1996)
Phys. Rev. D
, vol.54
, pp. 4131
-
-
Morningstar, C.J.1
Weinstein, M.2
-
10
-
-
85038307194
-
-
C. J. Morningstar and M. Weinstein, Phys. Rev. D 54, 4131 (1996). For Hubbard models, see E. Altman and A. Auerbach, Phys. Rev. B 65, 104508 (2002).
-
(2002)
Phys. Rev. B
, vol.65
, pp. 104508
-
-
Altman, E.1
Auerbach, A.2
-
11
-
-
0036870758
-
-
On the 2 × 24 ladder, 2 × 2 plaquette bosonic triplet and hole pair states are retained to construct a range 2 effective Hamiltonian. On the 2 × 16 ladder, additional one-hole fermionic plaquette states are also kept; S. Capponi and D. Poilblanc, Phys. Rev. B 66, 180503(R) (2002).
-
(2002)
Phys. Rev. B
, vol.66
-
-
Capponi, S.1
Poilblanc, D.2
-
12
-
-
0000211870
-
-
D. Poilblanc, D. J. Scalapino, and W. Hanke, Phys. Rev. B 52, 6796 (1995); D. Poilblanc et al., Phys. Rev. B 62, R14633 (2000).
-
(1995)
Phys. Rev. B
, vol.52
, pp. 6796
-
-
Poilblanc, D.1
Scalapino, D.J.2
Hanke, W.3
-
13
-
-
0034450735
-
-
D. Poilblanc, D. J. Scalapino, and W. Hanke, Phys. Rev. B 52, 6796 (1995); D. Poilblanc et al., Phys. Rev. B 62, R14633 (2000).
-
(2000)
Phys. Rev. B
, vol.62
-
-
Poilblanc, D.1
-
15
-
-
0242333567
-
-
The second charge mode is gapped
-
The second charge mode is gapped
-
-
-
-
16
-
-
0003345088
-
-
M. Troyer, H. Tsunetsugu, and T.M. Rice, Phys. Rev. B 53, 251 (1996); CA. Hayward and D. Poilblanc, Phys. Rev. B 53, 11 721 (1996).
-
(1996)
Phys. Rev. B
, vol.53
, pp. 251
-
-
Troyer, M.1
Tsunetsugu, H.2
Rice, T.M.3
-
17
-
-
0000754657
-
-
M. Troyer, H. Tsunetsugu, and T.M. Rice, Phys. Rev. B 53, 251 (1996); CA. Hayward and D. Poilblanc, Phys. Rev. B 53, 11 721 (1996).
-
(1996)
Phys. Rev. B
, vol.53
, pp. 11721
-
-
Hayward, C.A.1
Poilblanc, D.2
-
20
-
-
0000084186
-
-
Y. Ohta, T. Shimozato, R. Eder, and S. Maekawa, Phys. Rev. Lett. 73, 324 (1994).
-
(1994)
Phys. Rev. Lett.
, vol.73
, pp. 324
-
-
Ohta, Y.1
Shimozato, T.2
Eder, R.3
Maekawa, S.4
-
21
-
-
4444350611
-
-
-1/2Kp factor times a function of ω and q which is independent of L. E. Orignac and D. Poilblanc, Phys. Rev. B 68, 052504 (2003).
-
(2003)
Phys. Rev. B
, vol.68
, pp. 052504
-
-
Orignac, L.E.1
Poilblanc, D.2
-
22
-
-
0034900669
-
-
T. Siller, M. Troyer, T. M. Rice, and S. R. White, Phys. Rev. B 63, 195106 (2001).
-
(2001)
Phys. Rev. B
, vol.63
, pp. 195106
-
-
Siller, T.1
Troyer, M.2
Rice, T.M.3
White, S.R.4
-
23
-
-
85088489148
-
-
note
-
0, we have set ω = 0.
-
-
-
|