Mass deforming an N=2 superconformal theory with two different masses produces a third-order phase transition at finite 't Hooft coupling.
N=2* Super-Yang-Mills Theory at Strong Coupling
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The planar N=2* Super-Yang-Mills (SYM) theory is solved at large 't Hooft coupling using localization on S(4). The solution permits detailed investigation of the resonance phenomena responsible for quantum phase transitions in infinite volume, and leads to quantitative predictions for the semiclassical string dual of the N=2* theory.
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More on phase transitions in ${\cal N}$ = 2 massive gauge theories
Mass deforming an N=2 superconformal theory with two different masses produces a third-order phase transition at finite 't Hooft coupling.