THE CRUMPLING TRANSITION OF CRYSTALLINE RANDOM SURFACES
THE CRUMPLING TRANSITION OF CRYSTALLINE RANDOM SURFACES
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DOI:
10.1016/0550-3213(91)90166-u
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发表时间:
1991-02-25
影响因子:
2.8
通讯作者:
WHEATER, JF
中科院分区:
文献类型:
--
作者:
HARNISH, RG;WHEATER, JF
We investigate the crumpling transition in two different models of crystalline random surfaces with extrinsic curvature which have recently caused some confusion and find that many of the results previously obtained are erroneous. Using the Fourier acceleration technique to ameliorate critical slowing down problems we have made numerical simulations of surfaces of up to 128(2) points embedded in three dimensions. The first model, which has a non-compact lattice version of the extrinsic curvature, suffers from a sickness in the non-crumpled phase which is a lattice artefact; it is smooth in one intrinsic direction and folded up on the scale of the lattice spacing in the other, so we call this phase corrugated. The crumpling transition is continuous, having a diverging persistence length with critical exponent v = 1.15 +/- 0.15 and a cusp in the specific heat indicating that alpha less-than-or-equal-to 0. The second model, in which the extrinsic curvature depends upon the cosine of the angle between normals of adjacent triangles, also has a continuous transition with v = 0.94 +/- 0.20 and alpha = 0.53 +/- 0.15. Just beyond the crumpling transition, the smooth phase is found to have Hausdorff dimension d(H) < 2.14 at two standard deviations and so we conclude that d(H) = 2 throughout this phase. A study of the correlation functions shows that, in the crumpled phase, the system is apparently described by a very simple gaussian action. If true, this result could have important implications which we discuss briefly.