-
1
-
-
0023646228
-
-
SCIEAS 0036-8075 10.1016/S0921-4534(97)00266-9
-
P. W. Anderson, Science SCIEAS 0036-8075 10.1016/S0921-4534(97)00266-9 235, 1196 (1987).
-
(1987)
Science
, vol.235
, pp. 1196
-
-
Anderson, P.W.1
-
2
-
-
24544479379
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.37.3759
-
F. C. Zhang and T. M. Rice, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.37.3759 37, 3759 (1988).
-
(1988)
Phys. Rev. B
, vol.37
, pp. 3759
-
-
Zhang, F.C.1
Rice, T.M.2
-
3
-
-
12044251032
-
-
RMPHAT 0034-6861 10.1103/RevModPhys.66.763
-
E. Dagotto, Rev. Mod. Phys. RMPHAT 0034-6861 10.1103/RevModPhys.66.763 66, 763 (1994).
-
(1994)
Rev. Mod. Phys.
, vol.66
, pp. 763
-
-
Dagotto, E.1
-
4
-
-
0001457768
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.37.3664
-
G. Kotliar, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.37.3664 37, 3664 (1988). This state can also be written as a projected s+id spin liquid.
-
(1988)
Phys. Rev. B
, vol.37
, pp. 3664
-
-
Kotliar, G.1
-
5
-
-
2842611253
-
-
JUPSAU 0031-9015 10.1143/JPSJ.57.2482
-
H. Yokoyama and H. Shiba, J. Phys. Soc. Jpn. JUPSAU 0031-9015 10.1143/JPSJ.57.2482 57, 2482 (1988).
-
(1988)
J. Phys. Soc. Jpn.
, vol.57
, pp. 2482
-
-
Yokoyama, H.1
Shiba, H.2
-
6
-
-
0000440340
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.38.931
-
C. Gros, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.38.931 38, R931 (1988);
-
(1988)
Phys. Rev. B
, vol.38
, pp. 931
-
-
Gros, C.1
-
7
-
-
0035914763
-
-
for recent estimations see, e.g., PRLTAO 0031-9007 10.1103/PhysRevLett. 87.217002
-
for recent estimations see, e.g., A. Paramekanti, M. Randeria, and N. Trivedi, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.87.217002 87, 217002 (2001).
-
(2001)
Phys. Rev. Lett.
, vol.87
, pp. 217002
-
-
Paramekanti, A.1
Randeria, M.2
Trivedi, N.3
-
9
-
-
3042846888
-
-
JCOMEL 0953-8984 10.1088/0953-8984/16/24/R02
-
P. W. Anderson, P. A. Lee, M. Randeria, T. M. Rice, N. Trivedi, and F. C. Zhang, J. Phys.: Condens. Matter JCOMEL 0953-8984 10.1088/0953-8984/16/24/R02 16, R755 (2004).
-
(2004)
J. Phys.: Condens. Matter
, vol.16
, pp. 755
-
-
Anderson, P.W.1
Lee, P.A.2
Randeria, M.3
Rice, T.M.4
Trivedi, N.5
Zhang, F.C.6
-
10
-
-
0001185515
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.37.3774
-
I. Affleck and J. B. Marston, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.37.3774 37, R3774 (1988);
-
(1988)
Phys. Rev. B
, vol.37
, pp. 3774
-
-
Affleck, I.1
Marston, J.B.2
-
11
-
-
35949011942
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.39.11538
-
J. B. Marston and I. Affleck, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.39.11538 39, 11538 (1989).
-
(1989)
Phys. Rev. B
, vol.39
, pp. 11538
-
-
Marston, J.B.1
Affleck, I.2
-
12
-
-
19744382372
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.70.104503
-
D. A. Ivanov, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.70.104503 70, 104503 (2004) and references therein;
-
(2004)
Phys. Rev. B
, vol.70
, pp. 104503
-
-
Ivanov, D.A.1
-
13
-
-
0000860252
-
-
see also PRBMDO 0163-1829 10.1103/PhysRevB.41.6989
-
see also D. Poilblanc and Y. Hasegawa, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.41.6989 41, 6989 (1990).
-
(1990)
Phys. Rev. B
, vol.41
, pp. 6989
-
-
Poilblanc, D.1
Hasegawa, Y.2
-
14
-
-
0001567604
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.57.6003
-
P. A. Lee, N. Nagaosa, T. K. Ng, and X. G. Wen, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.57.6003 57, 6003 (1998).
-
(1998)
Phys. Rev. B
, vol.57
, pp. 6003
-
-
Lee, P.A.1
Nagaosa, N.2
Ng, T.K.3
Wen, X.G.4
-
15
-
-
4243394128
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.76.503
-
X. G. Wen and P. A. Lee, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.76.503 76, 503 (1996).
-
(1996)
Phys. Rev. Lett.
, vol.76
, pp. 503
-
-
Wen, X.G.1
Lee, P.A.2
-
16
-
-
0000668549
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.46.8434
-
M. U. Ubbens and P. A. Lee, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.46.8434 46, 8434 (1992).
-
(1992)
Phys. Rev. B
, vol.46
, pp. 8434
-
-
Ubbens, M.U.1
Lee, P.A.2
-
17
-
-
0001032458
-
-
PLRBAQ 0556-2805 10.1103/PhysRevB.14.2239
-
D. R. Hofstadter, Phys. Rev. B PLRBAQ 0556-2805 10.1103/PhysRevB.14.2239 14, 2239 (1976).
-
(1976)
Phys. Rev. B
, vol.14
, pp. 2239
-
-
Hofstadter, D.R.1
-
19
-
-
33644549091
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.40.7376
-
D. Poilblanc, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.40.7376 40, R 7376 (1989);
-
(1989)
Phys. Rev. B
, vol.40
, pp. 7376
-
-
Poilblanc, D.1
-
21
-
-
0642351853
-
-
for related results using slave boson MF techniques see, e.g., PRBMDO 0163-1829 10.1103/PhysRevB.41.7277
-
for related results using slave boson MF techniques see, e.g., F. Nori, E. Abrahams, and G. T. Zimanyi, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.41.7277 41, R 7277 (1990).
-
(1990)
Phys. Rev. B
, vol.41
, pp. 7277
-
-
Nori, F.1
Abrahams, E.2
Zimanyi, G.T.3
-
23
-
-
1642294555
-
-
SCIEAS 0036-8075 10.1126/science.1093384
-
M. Vershinin, S. Misra, S. Ono, Y. Abe, Y. Ando, and A. Yazdani, Science SCIEAS 0036-8075 10.1126/science.1093384 303, 1995 (2004).
-
(2004)
Science
, vol.303
, pp. 1995
-
-
Vershinin, M.1
Misra, S.2
Ono, S.3
Abe, Y.4
Ando, Y.5
Yazdani, A.6
-
24
-
-
0037127057
-
-
Note that the first observation was made around a vortex core in SCIEAS 0036-8075 10.1126/science.1066974
-
Note that the first observation was made around a vortex core in J. E. Hoffman, E. W. Hudson, K. M. Lang, V. Madhavan, H. Eisaki, S. Uchida, and J. C. Davis, Science SCIEAS 0036-8075 10.1126/science.1066974 295, 466 (2002).
-
(2002)
Science
, vol.295
, pp. 466
-
-
Hoffman, J.E.1
Hudson, E.W.2
Lang, K.M.3
Madhavan, V.4
Eisaki, H.5
Uchida, S.6
Davis, J.C.7
-
25
-
-
0037119614
-
-
Note that the energy-dependent spatial modulations of the tunneling conductance of optimally doped BSCO can be understood in terms of elastic scattering of quasiparticles; see SCIEAS 0036-8075
-
Note that the energy-dependent spatial modulations of the tunneling conductance of optimally doped BSCO can be understood in terms of elastic scattering of quasiparticles; see J. E. Hoffman, K. McElroy, D. H. Lee, K. M. Lang, H. Eisaki, S. Uchida, and J. C. Davis, Science SCIEAS 0036-8075 297, 1148 (2002).
-
(2002)
Science
, vol.297
, pp. 1148
-
-
Hoffman, J.E.1
McElroy, K.2
Lee, D.H.3
Lang, K.M.4
Eisaki, H.5
Uchida, S.6
Davis, J.C.7
-
26
-
-
29144498011
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.95.257005
-
G. Levy, M. Kugler, A. A. Manuel, O. Fischer, and M. Li, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.95.257005 95, 257005 (2005).
-
(2005)
Phys. Rev. Lett.
, vol.95
, pp. 257005
-
-
Levy, G.1
Kugler, M.2
Manuel, A.A.3
Fischer, O.4
Li, M.5
-
28
-
-
4344605135
-
-
NATUAS 0028-0836 10.1038/nature02861
-
T. Hanaguri, Nature (London) NATUAS 0028-0836 10.1038/nature02861 430, 1001 (2004).
-
(2004)
Nature (London)
, vol.430
, pp. 1001
-
-
Hanaguri, T.1
-
29
-
-
33744619385
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.10.159
-
M. C. Gutzwiller, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett. 10.159 10, 159 (1963);
-
(1963)
Phys. Rev. Lett.
, vol.10
, pp. 159
-
-
Gutzwiller, M.C.1
-
30
-
-
35949016490
-
-
RMPHAT 0034-6861 10.1103/RevModPhys.56.99
-
D. Vollhardt, Rev. Mod. Phys. RMPHAT 0034-6861 10.1103/RevModPhys.56.99 56, 99 (1984).
-
(1984)
Rev. Mod. Phys.
, vol.56
, pp. 99
-
-
Vollhardt, D.1
-
31
-
-
0007690360
-
-
SUSTEF 0953-2048 10.1088/0953-2048/1/1/009
-
F. C. Zhang, C. Gros, T. M. Rice, and H. Shiba, Supercond. Sci. Technol. SUSTEF 0953-2048 10.1088/0953-2048/1/1/009 1, 36 (1988).
-
(1988)
Supercond. Sci. Technol.
, vol.1
, pp. 36
-
-
Zhang, F.C.1
Gros, C.2
Rice, T.M.3
Shiba, H.4
-
32
-
-
33644554747
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.41.4827
-
D. Poilblanc, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.41.4827 41, R 4827 (1990); note that, in this early treatment, uniform Gutzwiller parameters were assumed although the phases of the bond variables were allowed to vary spatially.
-
(1990)
Phys. Rev. B
, vol.41
, pp. 4827
-
-
Poilblanc, D.1
-
33
-
-
33644540213
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.72.060508
-
D. Poilblanc, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.72.060508 72, 060508 (R) (2005).
-
(2005)
Phys. Rev. B
, vol.72
, pp. 060508
-
-
Poilblanc, D.1
-
34
-
-
33748708996
-
-
cond-mat/0406038 (unpublished);
-
Such a formulation should be appropriate as long as the deviations of ni from the average density remain small. See P. W. Anderson, cond-mat/0406038 (unpublished);
-
-
-
Anderson, P.W.1
-
35
-
-
33748706525
-
-
cond-mat/0312573 (unpublished).
-
B. A. Bernevig, cond-mat/0312573 (unpublished).
-
-
-
Bernevig, B.A.1
-
36
-
-
33144466567
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.73.060501
-
C. Li, S. Zhou, and Z. Wang, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.73.060501 73, 060501 (R) (2006).
-
(2006)
Phys. Rev. B
, vol.73
, pp. 060501
-
-
Li, C.1
Zhou, S.2
Wang, Z.3
-
37
-
-
4243459700
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.42.8690
-
Z. Wang, G. Kotliar, and X. F. Wang, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.42.8690 42, R 8690 (1990); note that the Fermi surface of the SFP is made of four small ellipticlike pockets centered around (±π 2,±π 2).
-
(1990)
Phys. Rev. B
, vol.42
, pp. 8690
-
-
Wang, Z.1
Kotliar, G.2
Wang, X.F.3
-
38
-
-
0034261241
-
-
Also found in SU (2N) mean-field theory; see PRBMDO 0163-1829 10.1103/PhysRevB.62.6721
-
Also found in SU (2N) mean-field theory; see M. Vojta, Y. Zhang, and S. Sachdev, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.62.6721 62, 6721 (2000), and references therein.
-
(2000)
Phys. Rev. B
, vol.62
, pp. 6721
-
-
Vojta, M.1
Zhang, Y.2
Sachdev, S.3
-
39
-
-
0036753363
-
-
Our 4×4 solution bears some similarities with those obtained within SU (2N) Sp (2N) mean-field theories; see 10.1103/PhysRevB.66.104505 0163-1829 PRBMDO
-
Our 4×4 solution bears some similarities with those obtained within SU (2N) Sp (2N) mean-field theories; see M. Vojta, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.66.104505 66, 104505 (2002). Note, however, that the large- N Sp (2N) scheme implies a superconducting state.
-
(2002)
Phys. Rev. B
, vol.66
, pp. 104505
-
-
Vojta, M.1
-
40
-
-
36149021666
-
-
PHRVAO 0031-899X 10.1103/PhysRev.98.1479
-
R. Jastrow, Phys. Rev. PHRVAO 0031-899X 10.1103/PhysRev.98.1479 98, 1479 (1955).
-
(1955)
Phys. Rev.
, vol.98
, pp. 1479
-
-
Jastrow, R.1
|