1996
DOI: 10.1016/0550-3213(96)00360-4
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Algebraic renormalization of N = 1 supersymmetric gauge theories with supersymmetry breaking masses

Abstract: We provide N = 1 Super Yang-Mills theory in the Wess-Zumino gauge with mass terms for the supersymmetric partners of the gauge fields and of the matter fields, together with a supersymmetric mass term for the fermionic matter fields. All mass terms are chosen in such a way to induce soft supersymmetry breakings at most, while preserving gauge invariance to all orders of perturbation theory. The breakings are controlled through an extended Slavnov-Taylor identity. The renormalization analysis, both in the ultra… Show more

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Cited by 32 publications
(81 citation statements)
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“…For the standard model the algebraic renormalization has been worked out in [22], soft breakings have been introduced in [23]. Although the corresponding Slavnov-Taylor identities are more involved since they have to express not only the symmetries but also the spontaneous or soft breaking, their structure is the same as in SQED.…”
Section: Discussionmentioning
confidence: 99%
“…For the standard model the algebraic renormalization has been worked out in [22], soft breakings have been introduced in [23]. Although the corresponding Slavnov-Taylor identities are more involved since they have to express not only the symmetries but also the spontaneous or soft breaking, their structure is the same as in SQED.…”
Section: Discussionmentioning
confidence: 99%
“…See Refs. [49,50,51] and references therein. The onshell closure can also be incorporated into this framework by introducing a term that is quadratic in the "anti-field" of the gluino, K ψ (see, for example, Refs.…”
Section: General Frameworkmentioning
confidence: 99%
“…If one wants to constrain the structure of radiative corrections by using the Slavnov-Taylor (ST) identity or the Zinn-Justin equation, those relations should not contain tree-level symmetry-breakings such as the gluino mass term. To circumvent this point, we introduce generalized BRS doublet fields (spurions) (u V , v V ) and (u A , v A ) which make the mass term "formally" BRS invariant [71,51].…”
Section: General Frameworkmentioning
confidence: 99%
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