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116 (1984) 2 5 1 , and references t h e r e i n . 11) G. V e n e z i a n o , N u c l . P h y s . B 1 5 9 ( 1 9 7 9 ) 213. 1 2 ) P. Di V e c c h i a , K . F a b r i c i u s , G . C . R o s s i a n d G . V e n e z i a n o , N u c l . P h y s . B 1 9 2 (1981) 392 and Phys. Lett. J. P o l o n y i , P h y s . R e v . D 2 9 ( 1 9 8 4 ) 7 1 6 ; Y. Iwasaki and T. Y o s h i e \ P h y s . L e t t . 131B ( 1 9 8 3 ) 1 5 9 ; P. W o i t , P h y s . R e v . L e t t . 51 ( 1 9 8 2 ) 6 3 8 ; I . A . F o x , J .

They include terms that generalize those required b y the U^(1) anomaly in QCD. Some o f these Lagrangians have been written for a number o f theories. (SS*) / 1 ^[S log(S/A ) - S + h . 1) 3 3 R a that satisfies the anomalous Ward identities o f super Yang-Mills theory. 1) one gets gluino condensation that isalso confirmed b y some 21 2 2 instanton exact calculation In t h e p u r e N = 2 Y a n g - M i l l s t h e o r y a n o b v i o u s c o n d e n s a t e i s R = where now W is the N = 2 superfield strength.

Ellwanger, N u c l . Phys. B245 (1984) 237. 29) A . C. Davis, P. Di Vecchia and P. Salomonson, Nucl. Phys. (1983) 45. K. Nielsen, Nucl. Phys. B244 (1984) 499. G u a d a g n i n i , K. Konishi and M. M i n t c h e v , University o f Pisa IFUP T H - 1 o / 8 5 . K. Nielsen, University o f Odense preprint (1985) 33) D . Nemeschansky and R . Rohm, Nucl. Phys. B249 (1985) 157; see also E. Cohen and C. G o m e z , CERN preprint T H 4 o 4 3 / 8 4 . preprint RECENT DEVELOPMENTS Q UANTUM FIELD THEOR J. J.

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