Academic Journal
and
العنوان: | and |
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المؤلفون: | Kenichi Konishi, Antonio Ricco |
المساهمون: | The Pennsylvania State University CiteSeerX Archives |
المصدر: | http://arxiv.org/pdf/hep-th/0306128v1.pdf. |
سنة النشر: | 2003 |
المجموعة: | CiteSeerX |
الوصف: | We determine the gluino condensate 〈 Trλ 2 〉 in the pure N = 1 super Yang-Mills theory (SYM) for the classical gauge groups SU(r+1), SO(2r+1), USp(2r) and SO(2r), by deforming the pure N = 2 SYM theory with the adjoint scalar multiplet mass, following the work by Finnell and Pouliot, and Ritz and Vainshtein. The value of the gluino condensate agrees in all cases with what was found in the weak coupling istanton calculation. The value of the gluino condensate in the pure N = 1 super Yang-Mills theory with gauge group SU(r + 1) has been calculated in the eighties by using two different methods. In the first one [1], called the strong coupling instanton calculation, one evaluates the (r+1) point function 〈 Trλ 2 (x1). Trλ 2 (xr+1) 〉 which is saturated by one instanton zero modes at short distances, and being constant due to supersymmetric Ward-Takahashi identities, it is set equal to the product of 〈 Trλ 2 〉 by clustering. The second method [2], the so-called weak coupling istanton calculation, makes use of a deformation of the original theory by addition of some matter fields. Classically, the |
نوع الوثيقة: | text |
وصف الملف: | application/pdf |
اللغة: | English |
Relation: | http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.264.6630; http://arxiv.org/pdf/hep-th/0306128v1.pdf |
الاتاحة: | http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.264.6630 http://arxiv.org/pdf/hep-th/0306128v1.pdf |
Rights: | Metadata may be used without restrictions as long as the oai identifier remains attached to it. |
رقم الانضمام: | edsbas.1FEBE81A |
قاعدة البيانات: | BASE |
الوصف غير متاح. |