Computational Physics 1996
DOI: 10.1007/978-3-642-85238-1_3
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Monte Carlo Simulations of Spin Systems

Abstract: Abstract. This lecture gives a brief introduction to Monte Carlo simulations of classical O(n) spin systems such as the Ising (n = 1), XY (n = 2), and Heisenberg (n = 3) model. In the first part I discuss some aspects of Monte Carlo algorithms to generate the raw data. Here special emphasis is placed on non-local cluster update algorithms which proved to be most efficient for this class of models. The second part is devoted to the data analysis at a continuous phase transition. For the example of the three-dim… Show more

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Cited by 31 publications
(36 citation statements)
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“…However, a single-cluster variant can also be implemented with strictly O(N) run-time scaling and is hence found to be asymptotically more efficient than Luijten's approach. For the simulations close to criticality, we determine integrated autocorrelation times to ensure equilibration and sufficient independence of successive samples [35]. Our simulations indicate a dramatic reduction of autocorrelation times and also the dynamical critical exponents through the use of the cluster updates.…”
Section: Cluster-update Monte Carlo Simulationsmentioning
confidence: 99%
“…However, a single-cluster variant can also be implemented with strictly O(N) run-time scaling and is hence found to be asymptotically more efficient than Luijten's approach. For the simulations close to criticality, we determine integrated autocorrelation times to ensure equilibration and sufficient independence of successive samples [35]. Our simulations indicate a dramatic reduction of autocorrelation times and also the dynamical critical exponents through the use of the cluster updates.…”
Section: Cluster-update Monte Carlo Simulationsmentioning
confidence: 99%
“…Hence, the plaquette update simulates the (transcribed) dual rather than the original model itself. Figure 7 gives the exact internal energy of the original Ising model on a finite lattice with periodic boundary conditions [39,40] and that of the dual model transcribed to the original one using Eq. (38).…”
Section: Monte Carlo Studymentioning
confidence: 99%
“…where the constant t defines the characteristic length scale at which the environmental response changes, known as the correlation length (Janke 1996). To model environmental variation in both space and time, we generate U j, x (t) with a two-parameter autoregressive process ("Modeling Details"), which introduces both spatial and temporal correlation lengths.…”
Section: Model Of Stream Communitiesmentioning
confidence: 99%