Hyperscaling Violation in Ising Spin Glasses
In addition to the standard scaling rules relating critical exponents at second order transitions, hyperscaling rules involve the dimension of the model. It is well known that in canonical Ising models hyperscaling rules are modified above the upper critical dimension. It was shown by M. Schwartz in...
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doaj-0f713f6a039a4acbb329a8acd90e120d2020-11-25T01:27:37ZengMDPI AGEntropy1099-43002019-10-01211097810.3390/e21100978e21100978Hyperscaling Violation in Ising Spin GlassesIan A. Campbell0Per H. Lundow1Laboratoire Charles Coulomb (L2C), UMR 5221 CNRS-Université de Montpellier, 34095 Montpellier, FranceDepartment of Mathematics and Mathematical Statistics, Umeå University, SE-901 87 Umeå, SwedenIn addition to the standard scaling rules relating critical exponents at second order transitions, hyperscaling rules involve the dimension of the model. It is well known that in canonical Ising models hyperscaling rules are modified above the upper critical dimension. It was shown by M. Schwartz in 1991 that hyperscaling can also break down in Ising systems with quenched random interactions; Random Field Ising models, which are in this class, have been intensively studied. Here, numerical Ising Spin Glass data relating the scaling of the normalized Binder cumulant to that of the reduced correlation length are presented for dimensions 3, 4, 5, and 7. Hyperscaling is clearly violated in dimensions 3 and 4, as well as above the upper critical dimension <inline-formula> <math display="inline"> <semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>6</mn> </mrow> </semantics> </math> </inline-formula>. Estimates are obtained for the “violation of hyperscaling exponent” values in the various models.https://www.mdpi.com/1099-4300/21/10/978spin glassesrandom interactionsscalinghyperscaling |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Ian A. Campbell Per H. Lundow |
spellingShingle |
Ian A. Campbell Per H. Lundow Hyperscaling Violation in Ising Spin Glasses Entropy spin glasses random interactions scaling hyperscaling |
author_facet |
Ian A. Campbell Per H. Lundow |
author_sort |
Ian A. Campbell |
title |
Hyperscaling Violation in Ising Spin Glasses |
title_short |
Hyperscaling Violation in Ising Spin Glasses |
title_full |
Hyperscaling Violation in Ising Spin Glasses |
title_fullStr |
Hyperscaling Violation in Ising Spin Glasses |
title_full_unstemmed |
Hyperscaling Violation in Ising Spin Glasses |
title_sort |
hyperscaling violation in ising spin glasses |
publisher |
MDPI AG |
series |
Entropy |
issn |
1099-4300 |
publishDate |
2019-10-01 |
description |
In addition to the standard scaling rules relating critical exponents at second order transitions, hyperscaling rules involve the dimension of the model. It is well known that in canonical Ising models hyperscaling rules are modified above the upper critical dimension. It was shown by M. Schwartz in 1991 that hyperscaling can also break down in Ising systems with quenched random interactions; Random Field Ising models, which are in this class, have been intensively studied. Here, numerical Ising Spin Glass data relating the scaling of the normalized Binder cumulant to that of the reduced correlation length are presented for dimensions 3, 4, 5, and 7. Hyperscaling is clearly violated in dimensions 3 and 4, as well as above the upper critical dimension <inline-formula> <math display="inline"> <semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>6</mn> </mrow> </semantics> </math> </inline-formula>. Estimates are obtained for the “violation of hyperscaling exponent” values in the various models. |
topic |
spin glasses random interactions scaling hyperscaling |
url |
https://www.mdpi.com/1099-4300/21/10/978 |
work_keys_str_mv |
AT ianacampbell hyperscalingviolationinisingspinglasses AT perhlundow hyperscalingviolationinisingspinglasses |
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