-
1
-
-
0347603892
-
-
For a review of possible quantum phases, see 10.1007/s00023-003-0948-4
-
For a review of possible quantum phases, see S. Sachdev, Ann. Henri Poincare 4, 637 (2003). 10.1007/s00023-003-0948-4
-
(2003)
Ann. Henri Poincare
, vol.4
, pp. 637
-
-
Sachdev, S.1
-
4
-
-
0242595882
-
-
10.1103/PhysRevB.68.115413
-
X.-G. Wen, Phys. Rev. B 68, 115413 (2003). 10.1103/PhysRevB.68.115413
-
(2003)
Phys. Rev. B
, vol.68
, pp. 115413
-
-
Wen, X.-G.1
-
5
-
-
33644502924
-
-
10.1103/PhysRevB.72.064455
-
C. Xu and J. E. Moore, Phys. Rev. B 72, 064455 (2005). 10.1103/PhysRevB.72.064455
-
(2005)
Phys. Rev. B
, vol.72
, pp. 064455
-
-
Xu, C.1
Moore, J.E.2
-
6
-
-
34848856711
-
-
10.1103/PhysRevB.76.104427
-
C. Xu and J. E. Moore, Phys. Rev. B 76, 104427 (2007). 10.1103/PhysRevB.76.104427
-
(2007)
Phys. Rev. B
, vol.76
, pp. 104427
-
-
Xu, C.1
Moore, J.E.2
-
7
-
-
33847223044
-
-
10.1103/PhysRevB.75.075116
-
M. Levin and X.-G. Wen, Phys. Rev. B 75, 075116 (2007). 10.1103/PhysRevB.75.075116
-
(2007)
Phys. Rev. B
, vol.75
, pp. 075116
-
-
Levin, M.1
Wen, X.-G.2
-
8
-
-
26144434509
-
-
10.1016/0550-3213(77)90086-4
-
A. M. Polyakov, Nucl. Phys. B 120, 429 (1977). 10.1016/0550-3213(77) 90086-4
-
(1977)
Nucl. Phys. B
, vol.120
, pp. 429
-
-
Polyakov, A.M.1
-
9
-
-
19744381248
-
-
10.1103/PhysRevB.70.100410
-
K. Louis and C. Gros, Phys. Rev. B 70, 100410 (R) (2004). 10.1103/PhysRevB.70.100410
-
(2004)
Phys. Rev. B
, vol.70
, pp. 100410
-
-
Louis, K.1
Gros, C.2
-
10
-
-
0000715040
-
-
10.1103/PhysRevB.59.R14157;
-
A. W. Sandvik, Phys. Rev. B 59, R14157 (1999) 10.1103/PhysRevB.59.R14157
-
(1999)
Phys. Rev. B
, vol.59
, pp. 14157
-
-
Sandvik, A.W.1
-
12
-
-
63249107587
-
-
On the time scale of our quantum Monte Carlo simulations, the system stays in one of the six degenerate symmetry-broken states. However, the finite-size system should fluctuate between different degenerate states on much longer Monte Carlo time scales.
-
On the time scale of our quantum Monte Carlo simulations, the system stays in one of the six degenerate symmetry-broken states. However, the finite-size system should fluctuate between different degenerate states on much longer Monte Carlo time scales.
-
-
-
-
13
-
-
33749473330
-
-
10.1103/PhysRevLett.97.147202
-
S. V. Isakov, S. Wessel, R. G. Melko, K. Sengupta, and Y. B. Kim, Phys. Rev. Lett. 97, 147202 (2006). 10.1103/PhysRevLett.97.147202
-
(2006)
Phys. Rev. Lett.
, vol.97
, pp. 147202
-
-
Isakov, S.V.1
Wessel, S.2
Melko, R.G.3
Sengupta, K.4
Kim, Y.B.5
-
14
-
-
33746928817
-
-
10.1103/PhysRevLett.97.067202
-
K. Damle and T. Senthil, Phys. Rev. Lett. 97, 067202 (2006). 10.1103/PhysRevLett.97.067202
-
(2006)
Phys. Rev. Lett.
, vol.97
, pp. 067202
-
-
Damle, K.1
Senthil, T.2
-
16
-
-
0034896225
-
-
10.1103/PhysRevB.63.224401
-
R. Moessner and S. L. Sondhi, Phys. Rev. B 63, 224401 (2001). 10.1103/PhysRevB.63.224401
-
(2001)
Phys. Rev. B
, vol.63
, pp. 224401
-
-
Moessner, R.1
Sondhi, S.L.2
|