Argues that confinement phases in 3d N=2 exceptional gauge theories have a single Coulomb branch, associated with quantum-deformed moduli spaces of corresponding 4d N=1 theories.
From 4D t o 3D chiral theories: Dressing the monopoles
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Confinement in 3d $\mathcal{N}=2$ exceptional gauge theories
Argues that confinement phases in 3d N=2 exceptional gauge theories have a single Coulomb branch, associated with quantum-deformed moduli spaces of corresponding 4d N=1 theories.