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Chernyak","submitted_at":"2016-03-14T13:30:10Z","abstract_excerpt":"Considered are ${\\cal N}=2\\, SU(N_c)$ or $U(N_c)$ SQCD with $N_F<2N_c-1$ quark flavors with the quark mass term $m{\\rm Tr}\\,({\\bar Q} Q)$ in the superpotential. ${\\cal N}=2$ supersymmetry is softly broken down to ${\\cal N}=1$ by the mass term $\\mu_{\\rm x}{\\rm Tr}\\,(X^2)$ of colored adjoint scalar partners of gluons, $\\mu_{\\rm x}\\ll\\Lambda_2$ ($\\Lambda_2$ is the scale factor of the $SU(N_c)$ gauge coupling).\n  There is a large number of different types of vacua in these theories with both unbroken and spontaneously broken flavor symmetry, $U(N_F)\\rightarrow U({\\rm n}_1)\\times U({\\rm n}_2)$. 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