TY - JOUR
T1 - Dynamic critical behavior of the Swendsen - Wang algorithm for the three-dimensional Ising model
AU - Ossola, Giovanni
AU - Sokal, Alan D.
N1 - Funding Information:
This research was supported in part by U.S. National Science Foundation Grants PHY-0099393 and PHY-0116590.
PY - 2004/7/26
Y1 - 2004/7/26
N2 - We have performed a high-precision Monte Carlo study of the dynamic critical behavior of the Swendsen-Wang algorithm for the three-dimensional Ising model at the critical point. For the dynamic critical exponents associated to the integrated autocorrelation times of the "energy-like" observables, we find zint,N=zint,E= zint,E′=0.459±0.005±0.025, where the first error bar represents statistical error (68% confidence interval) and the second error bar represents possible systematic error due to corrections to scaling (68% subjective confidence interval). For the "susceptibility-like" observables, we find zint,M2=zint, S2=0.443±0.005±0.030. For the dynamic critical exponent associated to the exponential autocorrelation time, we find zexp≈0.481. Our data are consistent with the Coddington-Baillie conjecture zSW=β/ν≈0.5183, especially if it is interpreted as referring to zexp.
AB - We have performed a high-precision Monte Carlo study of the dynamic critical behavior of the Swendsen-Wang algorithm for the three-dimensional Ising model at the critical point. For the dynamic critical exponents associated to the integrated autocorrelation times of the "energy-like" observables, we find zint,N=zint,E= zint,E′=0.459±0.005±0.025, where the first error bar represents statistical error (68% confidence interval) and the second error bar represents possible systematic error due to corrections to scaling (68% subjective confidence interval). For the "susceptibility-like" observables, we find zint,M2=zint, S2=0.443±0.005±0.030. For the dynamic critical exponent associated to the exponential autocorrelation time, we find zexp≈0.481. Our data are consistent with the Coddington-Baillie conjecture zSW=β/ν≈0.5183, especially if it is interpreted as referring to zexp.
KW - Autocorrelation time
KW - Cluster algorithm
KW - Dynamic critical exponent
KW - Ising model
KW - Monte Carlo
KW - Potts model
KW - Swendsen-Wang algorithm
UR - http://www.scopus.com/inward/record.url?scp=3042608076&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=3042608076&partnerID=8YFLogxK
U2 - 10.1016/j.nuclphysb.2004.04.026
DO - 10.1016/j.nuclphysb.2004.04.026
M3 - Article
AN - SCOPUS:3042608076
SN - 0550-3213
VL - 691
SP - 259
EP - 291
JO - Nuclear Physics B
JF - Nuclear Physics B
IS - 3
ER -