Phase transitions between confinement and higgs phases in SQCD with quark flavors
arXiv:2402.09490
Abstract
Considered is the standard 4-dimensional SQCD with quark flavors with masses . {\bf The gauge invariant order parameter is introduced in \cite{ch1} distinguishing confinement (with ) and higgs (with ) phases}. Using a number of independent arguments for different variants of transition between the confinement and higgs regimes in these theories, it is shown that {\bf transitions between these regimes are not crossovers but the phase transitions}. In \cite{FS} the very special QCD theory with defective scalar "quarks" was considered by E.Fradkin and S.H.Shenker. The conclusion of \cite{FS} was that {\bf the transition between the confinement and higgs regimes is the analytic crossover}. And although the theory considered in \cite{FS} was very specific, the experience shows that up to now there is a widely spread opinion that this conclusion has general applicability. This model \cite{FS} is criticized in \cite{ch1},\cite{ch2} as incompatible with and very different from the standard non-SUSY QCD theory with standard scalar quarks with all their physical degrees of freedom. It is emphasized that this model \cite{FS} is really {\bf the Stuckelberg YM-theory with no dynamical electric quarks and massive all electric gluons with fixed by hands nonzero masses}. There is no genuine confinement in this theory, it stays permanently in the completely higgsed (i.e. condensed) by hands phase only. And this is a reason for a crossover in this theory. While in the theory with standard scalar quarks there is the phase transition between the confinement (at ) and higgs (at ) regimes.
8 pages. Talk given at the International Conference on Particle Physics and Cosmology (professor V.A. Rubakov memorial conference), October 02-07, 2023, Yerevan, Armenia.\\