Abstract

We investigate the phase transition of the four-dimensional single-component ${\ensuremath{\phi}}^{4}$ theory on the lattice using the tensor renormalization group method. We have examined the hopping parameter dependence of the bond energy and the vacuum condensation of the scalar field $⟨\ensuremath{\phi}⟩$ at a finite quartic coupling $\ensuremath{\lambda}$ on large volumes up to $V=102{4}^{4}$ in order to detect the spontaneous breaking of the ${\mathbb{Z}}_{2}$ symmetry. Our results show that the system undergoes the weak first-order phase transition at a certain critical value of the hopping parameter. We also make a comparative study of the three-dimensional ${\ensuremath{\phi}}^{4}$ theory and find that the properties of the phase transition are consistent with the universality class of the three-dimensional Ising model.

Highlights

  • The issue of the triviality of the four-dimensional (4d) φ4 theory has been a theoretical concern among particle physicists, because it is related to the scalar sector in the standard model [1,2,3,4,5,6,7,8,9,10,11,12,13]

  • We have examined the hopping parameter dependence of the bond energy and the vacuum condensation of the scalar field hφi at a finite quartic coupling λ on large volumes up to V 1⁄4 10244 in order to detect the spontaneous breaking of the Z2 symmetry

  • We investigate the phase transition of the 4d single-component φ4 theory with the quartic coupling λ and the hopping parameter κ, employing the anisotropic tensor renormalization group (TRG) (ATRG) algorithm [30], which was proposed to reduce the

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Summary

INTRODUCTION

The issue of the triviality of the four-dimensional (4d) φ4 theory has been a theoretical concern among particle physicists, because it is related to the scalar sector in the standard model [1,2,3,4,5,6,7,8,9,10,11,12,13]. Thanks to the above feature (ii), we have been allowed to enlarge the lattice volume up to V 1⁄4 10244, which is essentially identified as the thermodynamic limit, and found finite jumps for the internal energy and the magnetization as functions of temperature in the 4d Ising model [27]. These are characteristic features of the first-order phase transition.

FORMULATION AND NUMERICAL ALGORITHM
NUMERICAL RESULTS
SUMMARY AND OUTLOOK
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