Revisiting $O(N)$ $\sigma$ model at unphysical pion masses and high temperatures. II. The vacuum structure and thermal $\sigma$ pole trajectory with cross-channel improvements

TL;DR

This paper investigates the vacuum structure and thermal sigma pole trajectory of the $O(N)$ model at large $N$, revealing limitations at high temperature and pion mass, and exploring phase correspondence and cross-channel effects.

Contribution

It introduces a detailed analysis of the $O(N)$ model's vacuum and sigma pole behavior at finite temperature and pion mass, including cross-channel improvements and phase correspondence.

Findings

Vacuum shifts from upper to lower branch with increasing $m_$ and temperature.

Existence of tachyon pole and its running are discussed.

Thermal sigma pole trajectory resembles zero-temperature behavior with varying pion mass.

Abstract

The effective potential of the $O(N)$ model at large $N$ limit is reinvestigated with varying pion mass and temperature. For large pion masses and high temperatures, we find the phenomenologically favored vacuum, located on the upper branch of the double-branched effective potential for physical $m_\pi$, moves to the lower branch and becomes no longer a local minimum but a saddle point. The existence and running of the tachyon pole are also discussed. These phenomena indicate that the applicable energy range of $O(N)$ model is more and more limited as $m_\pi$ becoming larger and temperature going higher. With the effective coupling constant defined from the effective potential, the possible correspondence between the two branches of the effective potential and the two phases of the theory (distinguished by positive or negative coupling) is verified even with nonzero explicit symmetry breaking and at finite temperature. Also, we generalize the $N/D$ modified $O(N)$ model to study the thermal trajectory of the $\sigma$ pole with the cross-channel contributions considered and find the thermal $\sigma$ pole trajectory resembles its counterpart with varying pion mass at zero temperature.