{"title":"2D additive small-world network with distance-dependent interactions","authors":"R. A. Dumer, M. Godoy","doi":"arxiv-2409.02033","DOIUrl":null,"url":null,"abstract":"In this work, we have employed Monte Carlo calculations to study the Ising\nmodel on a 2D additive small-world network with long-range interactions\ndepending on the geometric distance between interacting sites. The network is\ninitially defined by a regular square lattice and with probability $p$ each\nsite is tested for the possibility of creating a long-range interaction with\nany other site that has not yet received one. Here, we used the specific case\nwhere $p=1$, meaning that every site in the network has one long-range\ninteraction in addition to the short-range interactions of the regular lattice.\nThese long-range interactions depend on a power-law form,\n$J_{ij}=r_{ij}^{-\\alpha}$, with the geometric distance $r_{ij}$ between\nconnected sites $i$ and $j$. In current two-dimensional model, we found that\nmean-field critical behavior is observed only at $\\alpha=0$. As $\\alpha$\nincreases, the network size influences the phase transition point of the\nsystem, i.e., indicating a crossover behavior. However, given the\ntwo-dimensional system, we found the critical behavior of the short-range\ninteraction at $\\alpha\\approx2$. Thus, the limitation in the number of\nlong-range interactions compared to the globally coupled model, as well as the\nform of the decay of these interactions, prevented us from finding a regime\nwith finite phase transition points and continuously varying critical exponents\nin $0<\\alpha<2$.","PeriodicalId":501520,"journal":{"name":"arXiv - PHYS - Statistical Mechanics","volume":"181 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Statistical Mechanics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.02033","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
In this work, we have employed Monte Carlo calculations to study the Ising
model on a 2D additive small-world network with long-range interactions
depending on the geometric distance between interacting sites. The network is
initially defined by a regular square lattice and with probability $p$ each
site is tested for the possibility of creating a long-range interaction with
any other site that has not yet received one. Here, we used the specific case
where $p=1$, meaning that every site in the network has one long-range
interaction in addition to the short-range interactions of the regular lattice.
These long-range interactions depend on a power-law form,
$J_{ij}=r_{ij}^{-\alpha}$, with the geometric distance $r_{ij}$ between
connected sites $i$ and $j$. In current two-dimensional model, we found that
mean-field critical behavior is observed only at $\alpha=0$. As $\alpha$
increases, the network size influences the phase transition point of the
system, i.e., indicating a crossover behavior. However, given the
two-dimensional system, we found the critical behavior of the short-range
interaction at $\alpha\approx2$. Thus, the limitation in the number of
long-range interactions compared to the globally coupled model, as well as the
form of the decay of these interactions, prevented us from finding a regime
with finite phase transition points and continuously varying critical exponents
in $0<\alpha<2$.