-
8
-
-
0001325385
-
-
Phys. Rev. BT. Barnes, E. Dagotto, J. Riera, and E.S. Swanson, 47, 3196 (1993).
-
(1993)
Phys. Rev. B
, vol.47
, pp. 3196
-
-
Barnes, T.1
Dagotto, E.2
Riera, J.3
Swanson, E.S.4
-
19
-
-
85038958002
-
-
cond-mat/9605075 (unpublished)
-
H.J. Schultz, cond-mat/9605075 (unpublished).
-
-
-
Schultz, H.J.1
-
23
-
-
85038906352
-
-
cond-mat/9806215 (unpublished)
-
M. Mostovoy and D. Khomskii, cond-mat/9806215 (unpublished).
-
-
-
Mostovoy, M.1
Khomskii, D.2
-
27
-
-
0000598728
-
-
F. Mila, B. Frischmuth, A. Deppeler, and M. Troyer, Phys. Rev. Lett. 82, 3697 (1999);
-
(1999)
Phys. Rev. Lett.
, vol.82
, pp. 3697
-
-
Mila, F.1
Frischmuth, B.2
Deppeler, A.3
Troyer, M.4
-
29
-
-
3442899816
-
-
Phys. Rev. Lett.P. Azaria, A.O. Gogolin, P. Lecheminant, and A.A. Nersesyan, 83, 624 (1999);
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 624
-
-
Azaria, P.1
Gogolin, A.O.2
Lecheminant, P.3
Nersesyan, A.A.4
-
32
-
-
0000090084
-
-
Y.Q. Li, M. Ma, D.N. Shi, and F.C. Zhang, Phys. Rev. Lett. 81, 3527 (1998).
-
(1998)
Phys. Rev. Lett.
, vol.81
, pp. 3527
-
-
Li, Y.Q.1
Ma, M.2
Shi, D.N.3
Zhang, F.C.4
-
33
-
-
0000939733
-
-
C. Itoi, Shaojin Qin, and I. Affleck, Phys. Rev. B 61, 6747 (2000)
-
C. Itoi, Shaojin Qin, and I. Affleck, Phys. Rev. B 61, 6747 (2000).
-
-
-
-
36
-
-
85038951873
-
-
A.K. Kolezhuk, H.-J Mikeska, and U. Schollwök, cond-mat/0008321 (unpublished)
-
A.K. Kolezhuk, H.-J Mikeska, and U. Schollwök, cond-mat/0008321 (unpublished).
-
-
-
-
42
-
-
0001585364
-
-
Han-Ting Wang, Jue-Lian Shen, and Zhao-Bin Su, Phys. Rev. B 56, 14 435 (1997);
-
Han-Ting Wang, Jue-Lian Shen, and Zhao-Bin Su, Phys. Rev. B 56, 14 435 (1997);
-
-
-
-
43
-
-
0001648448
-
-
Phys. Rev. BHan-Ting Wang, H.Q. Lin, and Jue-Lian Shen, 61, 4019 (2000)
-
Phys. Rev. BHan-Ting Wang, H.Q. Lin, and Jue-Lian Shen, 61, 4019 (2000).
-
-
-
-
44
-
-
85038920440
-
-
The remaining eigenstates are the (Formula presented) quadruplets (Formula presented) (Formula presented) (Formula presented) (Formula presented) (Formula presented), corresponding to the eigenstates of (Formula presented) (Formula presented) (Formula presented) (Formula presented). With these four states included, the spin operators are expressed as (Formula presented)(Formula presented)
-
The remaining eigenstates are the (Formula presented) quadruplets (Formula presented) (Formula presented) (Formula presented) (Formula presented) (Formula presented), corresponding to the eigenstates of (Formula presented) (Formula presented) (Formula presented) (Formula presented). With these four states included, the spin operators are expressed as (Formula presented)(Formula presented).
-
-
-
-
48
-
-
0001472865
-
-
E. Sorensen, I. Affleck, D. Augier, and D. Poilblanc, Phys. Rev. B 58, R14 701 (1998).
-
(1998)
Phys. Rev. B
, vol.58
, pp. R14 701
-
-
Sorensen, E.1
Affleck, I.2
Augier, D.3
Poilblanc, D.4
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