Restoring isotropy in a three-dimensional lattice model: the Ising universality class

We study a generalized Blume-Capel model on the simple cubic lattice. In addition to the nearest-neighbor coupling there is a next-to-next-to-nearest-neighbor coupling. In order to quantify spatial anisotropy, we determine the correlation length in the high-temperature phase of the model for three d...

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Main Author: Hasenbusch, Martin (Author)
Format: Article (Journal)
Language:English
Published: 26 July 2021
In: Physical review
Year: 2021, Volume: 104, Issue: 1, Pages: 1-17
ISSN:2469-9969
DOI:10.1103/PhysRevB.104.014426
Online Access:Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1103/PhysRevB.104.014426
Verlag, lizenzpflichtig, Volltext: https://link.aps.org/doi/10.1103/PhysRevB.104.014426
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Author Notes:Martin Hasenbusch

MARC

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520 |a We study a generalized Blume-Capel model on the simple cubic lattice. In addition to the nearest-neighbor coupling there is a next-to-next-to-nearest-neighbor coupling. In order to quantify spatial anisotropy, we determine the correlation length in the high-temperature phase of the model for three different spatial directions. It turns out that the spatial anisotropy depends very little on the dilution or crystal-field parameter D of the model and is essentially determined by the ratio of the nearest-neighbor and the next-to-next-to-nearest-neighbor coupling. This ratio is tuned such that the leading contribution to the spatial anisotropy is eliminated. Next we perform a finite-size scaling (FSS) study to tune D such that also the leading correction to scaling is eliminated. Based on this FSS study, we determine the critical exponents ν=0.62998(5) and η=0.036284(40), which are in nice agreement with the more accurate results obtained by using the conformal bootstrap method. Furthermore, we provide accurate results for fixed-point values of dimensionless quantities such as the Binder cumulant and for the critical couplings. These results provide the groundwork for broader studies of universal properties of the three-dimensional Ising universality class. 
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