(In)stability of the Higgs vacuum from the $\text{O}(N)$ model at large $N$

Abstract

The theory of an independent Higgs field is given by an $\text{O}(N)$ model with an $N$-component scalar $\vec{\varphi }$ and a quartic $\lambda (\vec{\varphi }\cdot \vec{\varphi }{)}^2$ potential when $N=4$. The phase structure of the theory can be studied analytically for all values of the coupling $\lambda$ using the large-$N$ limit, both at zero and finite temperature. However, authors in the 70s and 80s argued the theory at large $N$ was "sick" and "futile", and dismissed the theory. This was based on two points: (1) a failure to identify the stable phases and vacuum of the theory and (2) the issue of a negative bare coupling $\lambda <0$ in the UV. We provide evidence that the theory is not, in fact, "sick". Issue (2) is dealt with through the modern understanding of $\mathcal{P}\mathcal{T}$-symmetric non-Hermitian theories with "wrong-sign" couplings. Issue (1) is resolved by realizing that the true vacuum has no spontaneous symmetry breaking (SSB) and that the SSB phase only becomes preferred at high temperatures.

Comments: 6 pages, 2 figures, conference proceedings for ICHEP 2024