Abstract

Finite-size scaling is investigated in detail around the critical point in the heavy-quark region of nonzero temperature QCD. Numerical simulations are performed with large spatial volumes up to the aspect ratio $N_s/N_t=12$ at a fixed lattice spacing with $N_t=4$. We show that the Binder cumulant and the distribution function of the Polyakov loop follow the finite-size scaling in the $Z(2)$ universality class for large spatial volumes with $N_s/N_t \ge 9$, while, for $N_s/N_t \le 8$, the Binder cumulant becomes inconsistent with the $Z(2)$ scaling. To realize the large-volume simulations in the heavy-quark region, we adopt the hopping parameter expansion for the quark determinant: We generate gauge configurations using the leading order action including the Polyakov loop term for $N_t=4$, and incorporate the next-to-leading order effects in the measurements by the multipoint reweighting method. We find that the use of the leading-order configurations is crucially effective in suppressing the overlapping problem in the reweighting and thus reducing the statistical errors.

Highlights

  • One of the interesting features of the medium described by quantum chromodynamics (QCD) is the existence of phase transitions of various orders

  • We show that the Binder cumulant and the distribution function of the Polyakov loop follow the finite-size scaling in the Zð2Þ universality class for large spatial volumes with Ns=Nt ≥ 9, while, for Ns=Nt ≤ 8, the Binder cumulant becomes inconsistent with the Zð2Þ scaling

  • We studied the distribution function of the Polyakov loop and its cumulants around the critical point (CP) in the heavy quark region of QCD

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Summary

INTRODUCTION

One of the interesting features of the medium described by quantum chromodynamics (QCD) is the existence of phase transitions of various orders. In the heavy quark region, on lattices of Nt 1⁄4 6 and 8 with the aspect ratio Ns=Nt 1⁄4 6 and 8, the Binder cumulant B4 is reported to be consistent with the Zð2Þ FSS using data mostly in the crossover side, while data in the first order side as well as that on Nt 1⁄4 10 lattice show a deviation from the Zð2Þ FSS [31] These results suggest the necessity of performing numerical analyses with even larger spatial volumes and with high statistics. We show that the use of the LO action to generate configurations is quite effective in suppressing the overlapping problem of the reweighting method This is essential for carrying out simulations with large system volumes as studied in the present paper. In Appendix D, the convergence of the HPE is examined by comparing the Binder cumulants at the LO and the NLO

FINITE-SIZE SCALING
Hopping parameter expansion
Numerical implementation with HPE
Simulation parameters
Overlapping problem
Transition line
Binder cumulant
Mixing with energylike observable
Nf dependence
Scaling of distribution function
Gap between the two minima
Discussions
CONCLUSIONS
N c M chair N site x
NcMbentNsite

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