The proof is based on a combination of two ideas: Refers to the theories with the strong coupling regime. ![]() Let us emphasize that the assertion made above Symplectic and exceptional groups will be Below we will prove that theĬondensate (1) does appear in the theories with the unitary and orthogonal gauge Within the framework of the superstring approach. Proposal to use the condensate (1) for the supersymmetry (SUSY) breaking The issue of the gluino condensation has become of special importance after the Non-vanishing vacuum expectation value ( ~ ) appears dynamically,Īt present, there exist several well-known arguments in favour of the gluinoĬondensation some of them, however, refer only to the unitary groups (see below). That in such theories with gauge groups SU(N) and O(N) (with no matter) a ![]() In the present work we consider supersymmetric Yang-Mills theories and prove (TrAA) has N different values while for the orthogonal groups (N - 2) values. O(N), k is an integer number, T(G) is one half of the Dynkin index. Obtained, (TrhA)o = ~cexp(2~rik/T(G)) ~ 0, where fi'G is the scale parameter, G = SU(N) or Method for calculating the gluino condensate (TrAh) in such theories. We consider supersymmetric SU(N) and O(N) gauge theories without matter and propose a Cheremushkinskaya W., 25, 117 259 Moscow, USSR Institute of Theoretical and Experimental Physics, B. ![]() ON GLUINO CONDENSATION IN SUPERSYMMETRIC GAUGE THEORIES
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