-
12
-
-
85038973692
-
-
Y. M. Cho, J. B. Hong, and C. N. Yang (World Scientific, Singapore
-
R. B. Laughlin, in Proceedings of the Inauguration Conference of the Asia-Pacific Center for Theoretical Physics, edited by Y. M. Cho, J. B. Hong, and C. N. Yang (World Scientific, Singapore, 1998).
-
(1998)
Proceedings of the Inauguration Conference of the Asia-Pacific Center for Theoretical Physics
-
-
Laughlin, R.B.1
-
27
-
-
0037175989
-
-
A. Sudbø, E. Smørgrav, J. Smiseth, F. S. Nogueira, and J. Hove, Phys. Rev. Lett. 89, 226403 (2002).
-
(2002)
Phys. Rev. Lett.
, vol.89
, pp. 226403
-
-
Sudbø, A.1
Smørgrav, E.2
Smiseth, J.3
Nogueira, F.S.4
Hove, J.5
-
32
-
-
0000918322
-
-
c = 1/3, see, e.g
-
c = 1/3, see, e.g., A. K. Nguyen and A. Sudbø, Phys. Rev. B 57, 3123 (1998).
-
(1998)
Phys. Rev. B
, vol.57
, pp. 3123
-
-
Nguyen, A.K.1
Sudbø, A.2
-
33
-
-
0037282254
-
-
c = 0.333068(7), see
-
c = 0.333068(7), see T. Neuhaus, A. Rajantie, and K. Rummukainen, 67, 014525 (2003).
-
(2003)
Phys. Rev. B
, vol.67
, pp. 14525
-
-
Neuhaus, T.1
Rajantie, A.2
Rummukainen, K.3
-
38
-
-
0011584621
-
-
D. J. Amit, S. Elitzur, E. Rabinovici, and R. Savit, Nucl. Phys. B 210, 69 (1982).
-
(1982)
Nucl. Phys. B
, vol.210
, pp. 69
-
-
Amit, D.J.1
Elitzur, S.2
Rabinovici, E.3
Savit, R.4
-
42
-
-
0003490204
-
-
S. Das Sarma and A. Pinczuk (Wiley, New York
-
Perspectives in Quantum Hall Effects, edited by S. Das Sarma and A. Pinczuk (Wiley, New York, 1997).
-
(1997)
Perspectives in Quantum Hall Effects
-
-
-
45
-
-
0035924349
-
-
D. A. Bonn, J. C. Wynn, B. W. Gardner, Y.-J. Lin, R. Liang, W. N. Hardy, J. R. Kirtley, and K. A. Moler, Nature (London) 414, 887 (2001).
-
(2001)
Nature (London)
, vol.414
, pp. 887
-
-
Bonn, D.A.1
Wynn, J.C.2
Gardner, B.W.3
Lin, Y.-J.4
Liang, R.5
Hardy, W.N.6
Kirtley, J.R.7
Moler, K.A.8
-
46
-
-
25744466740
-
-
I. Affleck, Z. Zou, T. Hsu, and P. W. Anderson, Phys. Rev. B 38, 745 (1988).
-
(1988)
Phys. Rev. B
, vol.38
, pp. 745
-
-
Affleck, I.1
Zou, Z.2
Hsu, T.3
Anderson, P.W.4
-
49
-
-
35949019960
-
-
The loop-gas representation of the 3D XY model is (Formula presented). The 3D XY model is given by the case q = 0 in Eq. (2). From Eq. (7) when (Formula presented), open-ended vortex configurations are suppressed; the system reverts to the 3D XY model, cf. (Formula presented)
-
R. Savit, Rev. Mod. Phys. 52, 453 (1980). The loop-gas representation of the 3D XY model is (Formula presented). The 3D XY model is given by the case q = 0 in Eq. (2). From Eq. (7) when (Formula presented), open-ended vortex configurations are suppressed; the system reverts to the 3D XY model, cf. (Formula presented).
-
(1980)
Rev. Mod. Phys.
, vol.52
, pp. 453
-
-
Savit, R.1
-
61
-
-
33646634437
-
-
The generalized Ising model formulation of the 8-vertex square lattice model is also given in, e.g
-
The generalized Ising model formulation of the 8-vertex square lattice model is also given in, e.g., F. Y. Wu, Phys. Rev. B 4, 2314 (1971);
-
(1971)
Phys. Rev. B
, vol.4
, pp. 2314
-
-
Wu, F.Y.1
-
62
-
-
0001133275
-
-
Another planar model exhibiting power-law singularities in the specific heat with nonuniversal exponents, is the square lattice Ashkin-Teller model, which also features a four-spin coupling
-
Phys. Rev. B L. P. Kadanoff and F. Wegner, 4, 3989 (1971). Another planar model exhibiting power-law singularities in the specific heat with nonuniversal exponents, is the square lattice Ashkin-Teller model, which also features a four-spin coupling.
-
(1971)
Phys. Rev. B
, vol.4
, pp. 3989
-
-
Kadanoff, L.P.1
Wegner, F.2
-
63
-
-
85039017922
-
-
Ph.D. thesis, Norwegian University of Science and Technology
-
J. Hove, Ph.D. thesis, Norwegian University of Science and Technology, 2002.
-
(2002)
-
-
Hove, J.1
-
66
-
-
3442899273
-
-
The three-dimensional noncompact U(1) gauge theory with Chern-Simons term added, is another example of a fixed-line theory with nonuniversal exponents. However, in this case both parity and time-reversal symmetry are broken. See, for instance
-
The three-dimensional noncompact U(1) gauge theory with Chern-Simons term added, is another example of a fixed-line theory with nonuniversal exponents. However, in this case both parity and time-reversal symmetry are broken. See, for instance, W. Chen, M. P. A. Fisher, and Y.-S. Wu, Phys. Rev. B 48, 13 749 (1993);
-
(1993)
Phys. Rev. B
, vol.48
, pp. 13 749
-
-
Chen, W.1
Fisher, M.P.A.2
Wu, Y.-S.3
-
67
-
-
0001650980
-
-
Phys. Rev. B C. de Calan, A. P. C. Malbouisson, F. S. Nogueira, and N. F. Svaiter, 59, 554 (1999);
-
(1999)
Phys. Rev. B
, vol.59
, pp. 554
-
-
de Calan, C.1
Malbouisson, A.P.C.2
Nogueira, F.S.3
Svaiter, N.F.4
|