4.4 Article

Symmetries and strings of adjoint QCD2

Journal

JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 3, Pages -

Publisher

SPRINGER
DOI: 10.1007/JHEP03(2021)103

Keywords

Anomalies in Field and String Theories; Discrete Symmetries; Topological Field Theories; Confinement

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The study revisits the symmetries of massless two-dimensional adjoint QCD with gauge group SU(N) and uncovers non-invertible symmetries severely constraining possible infrared phases and massive excitations. The theory enforces deconfinement of the fundamental quark through these new symmetries and exhibits soft breaking when the adjoint quark has a small mass. Additionally, the research delves into the dynamics of adjoint QCD deformed by symmetric quartic fermion interactions, suggesting partial confinement for the deformed theory and discussing emergent supersymmetry at nonzero mass.
We revisit the symmetries of massless two-dimensional adjoint QCD with gauge group SU(N). The dynamics is not sufficiently constrained by the ordinary symmetries and anomalies. Here we show that the theory in fact admits similar to 2(2N) non-invertible symmetries which severely constrain the possible infrared phases and massive excitations. We prove that for all N these new symmetries enforce deconfinement of the fundamental quark. When the adjoint quark has a small mass, m MUCH LESS-THAN g(YM), the theory confines and the non-invertible symmetries are softly broken. We use them to compute analytically the k-string tension for N <= 5. Our results suggest that the k-string tension, T-k, is T-k similar to |m| sin(pi k/N) for all N. We also consider the dynamics of adjoint QCD deformed by symmetric quartic fermion interactions. These operators are not generated by the RG flow due to the non-invertible symmetries, thus violating the ordinary notion of naturalness. We conjecture partial confinement for the deformed theory by these four-fermion interactions, and prove it for SU(N <= 5) gauge theory. Comparing the topological phases at zero and large mass, we find that a massless particle ought to appear on the string for some intermediate nonzero mass, consistent with an emergent supersymmetry at nonzero mass. We also study the possible infrared phases of adjoint QCD allowed by the non-invertible symmetries, which we are able to do exhaustively for small values of N. The paper contains detailed reviews of ideas from fusion category theory that are essential for the results we prove.

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