The Critical Exponents of Crystalline Random Surfaces

We report on a high statistics numerical study of the crystalline random surface model with extrinsic curvature on lattices of up to $64^2$ points. The critical exponents at the crumpling transition are determined by a number of methods all of which are shown to agree within estimated errors. The co...

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Main Author: Wheater, J
Format: Journal article
Published: 1995
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author Wheater, J
author_facet Wheater, J
author_sort Wheater, J
collection OXFORD
description We report on a high statistics numerical study of the crystalline random surface model with extrinsic curvature on lattices of up to $64^2$ points. The critical exponents at the crumpling transition are determined by a number of methods all of which are shown to agree within estimated errors. The correlation length exponent is found to be $\nu=0.71(5)$ from the tangent-tangent correlation function whereas we find $\nu=0.73(6)$ by assuming finite size scaling of the specific heat peak and hyperscaling. These results imply a specific heat exponent $\alpha=0.58(10)$; this is a good fit to the specific heat on a $64^2$ lattice with a $\chi^2$ per degree of freedom of 1.7 although the best direct fit to the specific heat data yields a much lower value of $\alpha$. Our measurements of the normal-normal correlation functions suggest that the model in the crumpled phase is described by an effective field theory which deviates from a free field theory only by super-renormalizable interactions.
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spelling oxford-uuid:d028dcbb-988a-47d8-89ee-f6f0dfa305eb2022-03-27T07:47:59ZThe Critical Exponents of Crystalline Random SurfacesJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:d028dcbb-988a-47d8-89ee-f6f0dfa305ebSymplectic Elements at Oxford1995Wheater, JWe report on a high statistics numerical study of the crystalline random surface model with extrinsic curvature on lattices of up to $64^2$ points. The critical exponents at the crumpling transition are determined by a number of methods all of which are shown to agree within estimated errors. The correlation length exponent is found to be $\nu=0.71(5)$ from the tangent-tangent correlation function whereas we find $\nu=0.73(6)$ by assuming finite size scaling of the specific heat peak and hyperscaling. These results imply a specific heat exponent $\alpha=0.58(10)$; this is a good fit to the specific heat on a $64^2$ lattice with a $\chi^2$ per degree of freedom of 1.7 although the best direct fit to the specific heat data yields a much lower value of $\alpha$. Our measurements of the normal-normal correlation functions suggest that the model in the crumpled phase is described by an effective field theory which deviates from a free field theory only by super-renormalizable interactions.
spellingShingle Wheater, J
The Critical Exponents of Crystalline Random Surfaces
title The Critical Exponents of Crystalline Random Surfaces
title_full The Critical Exponents of Crystalline Random Surfaces
title_fullStr The Critical Exponents of Crystalline Random Surfaces
title_full_unstemmed The Critical Exponents of Crystalline Random Surfaces
title_short The Critical Exponents of Crystalline Random Surfaces
title_sort critical exponents of crystalline random surfaces
work_keys_str_mv AT wheaterj thecriticalexponentsofcrystallinerandomsurfaces
AT wheaterj criticalexponentsofcrystallinerandomsurfaces