-
11
-
-
85036136001
-
-
Let us stress that other predictions of the standard field theory seem to be varified by performing a finite size scaling analysis (see 5 and 6), but a fully consistent scaling, including good data collapse for the order parameter, has never been observed. See the criticisms to 5 and 6 in 10
-
Let us stress that other predictions of the standard field theory seem to be varified by performing a finite size scaling analysis (see 5 and 6), but a fully consistent scaling, including good data collapse for the order parameter, has never been observed. See the criticisms to 5 and 6 in 10.
-
-
-
-
13
-
-
84956227279
-
-
Note that the two temperature model is equivalent to the random DLG at criticality
-
Europhys. Lett.Z. Cheng, P. L. Garrido, J. L. Lebowitz, and J. L. Vallés, 14, 507 (1991). Note that the two temperature model is equivalent to the random DLG at criticality.
-
(1991)
Europhys. Lett.
, vol.14
, pp. 507
-
-
Cheng, Z.1
Garrido, P.L.2
Lebowitz, J.L.3
Vallés, J.L.4
-
15
-
-
0001702031
-
-
J. Marro, A. Achahbar, P. L. Garrido, and J. Marro, Phys. Rev. E 53, 6038 (1996).
-
(1996)
Phys. Rev. E
, vol.53
, pp. 6038
-
-
Marro, J.1
Achahbar, A.2
Garrido, P.L.3
Marro, J.4
-
19
-
-
0007182966
-
-
A combinatorial error in the original calculation was corrected after a comment by S. Caracciolo (see also 16
-
F. de los Santos and M. A. Muñoz, Phys. Rev. E 61, 1161 (2000). A combinatorial error in the original calculation was corrected after a comment by S. Caracciolo (see also 16).
-
(2000)
Phys. Rev. E
, vol.61
, pp. 1161
-
-
de los Santos, F.1
Muñoz, M.A.2
-
21
-
-
85036412458
-
-
e-printcond-mat/9912286
-
B. Schmittmann, H. K. Janssen, U. C. Taeuber, R. K. P. Zia, K.-t. Leung, and J. L. Cardy, e-print cond-mat/9912286.
-
-
-
Schmittmann, B.1
Janssen, H.K.2
Taeuber, U.C.3
Zia, R.K.P.4
Leung, K.-t.5
Cardy, J.L.6
-
22
-
-
0007032916
-
-
Addison-Wesley, Reading, MA
-
For a presentation of the entropic versus the energetic part of the Ginzburg-Landau theory, see G. Parisi, in Frontiers in Physics (Addison-Wesley, Reading, MA, 1988).
-
(1988)
Frontiers in Physics
-
-
Parisi, G.1
-
23
-
-
85036325654
-
-
The detailed calculation will be presented elsewhere
-
The detailed calculation will be presented elsewhere.
-
-
-
-
24
-
-
85036307737
-
-
Observe that in the absence of the new term isotropic naive scaling, (Formula presented) had to be assumed. In the present case, (Formula presented) is obtained by imposing the leading term in the parallel direction to be marginal at the critical dimension
-
Observe that in the absence of the new term isotropic naive scaling, (Formula presented) had to be assumed. In the present case, (Formula presented) is obtained by imposing the leading term in the parallel direction to be marginal at the critical dimension.
-
-
-
-
26
-
-
84956065804
-
-
See also 2, Sec. 6.1
-
B. Schmittmann, Europhys. Lett. 24, 109 (1993). See also 2, Sec. 6.1.
-
(1993)
Europhys. Lett.
, vol.24
, pp. 109
-
-
Schmittmann, B.1
-
27
-
-
85036334758
-
-
Note that results up to first order in epsilon coincide with those obtained in our previous paper 14, but here (Formula presented)
-
Note that results up to first order in epsilon coincide with those obtained in our previous paper 14, but here (Formula presented)
-
-
-
-
29
-
-
85036405936
-
-
The prediction for the exponent ν up to two loops is (Formula presented) Monte Carlo simulations yield values around 0.7 for the DLG 3, and (Formula presented) for the random DLG 2
-
The prediction for the exponent ν up to two loops is (Formula presented) Monte Carlo simulations yield values around 0.7 for the DLG 3, and (Formula presented) for the random DLG 2.
-
-
-
-
30
-
-
3543015244
-
-
S. Caracciolo, R. G. Edwards, S. G. Ferreira, A. Pelissetto, and A. D. Sokal, Phys. Rev. Lett. 74, 2969 (1995).
-
(1995)
Phys. Rev. Lett.
, vol.74
, pp. 2969
-
-
Caracciolo, S.1
Edwards, R.G.2
Ferreira, S.G.3
Pelissetto, A.4
Sokal, A.D.5
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