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Related papers: Supersymmetry, Ultraviolet Finiteness and Grand Un…

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A formulation of (non-anticommutative) N=1/2 supersymmetric U(N) gauge theory in noncommutative space is studied. We show that at one loop UV/IR mixing occurs. A generalization of Seiberg-Witten map to noncommutative and non-anticommutative…

High Energy Physics - Theory · Physics 2008-11-26 O. F. Dayi , L. T. Kelleyane

We review some aspects of the correspondence between analytic gauge invariants and supersymmetric flat directions for vanishing D-terms and propose a criterion to include the F-term constraints.

High Energy Physics - Theory · Physics 2007-05-23 Ph. Brax , C. A. Savoy

Structure of quantum corrections in ${\cal N}=1$ supersymmetric gauge theories is investigated in the case of using the regularization by higher covariant derivatives. It is demonstrated that this regularization allows revealing some…

High Energy Physics - Theory · Physics 2021-11-29 Konstantin Stepanyantz

We study phenomenological aspects of supersymmetric SU(5) grand unified theories with non-universal gaugino masses. For large tan beta, we investigate constraints from the requirement of successful electroweak symmetry breaking, the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Katri Huitu , Yoshiharu Kawamura , Tatsuo Kobayashi , Kai Puolamaki

Finite Unified Theories (FUTs) are N=1 supersymmetric Grand Unified Theories that can be made all-loop finite, leading to a severe reduction of the free parameters. We review the investigation of FUTs based on SU(5) in the context of…

High Energy Physics - Phenomenology · Physics 2009-02-02 S. Heinemeyer , M. Mondragon , G. Zoupanos

Finite Unified Theories (FUTs) are N=1 supersymmetric Grand Unified Theories that can be made all-loop finite. The requirement of all-loop finiteness leads to a severe reduction of the free parameters of the theory and, in turn, to a large…

High Energy Physics - Phenomenology · Physics 2007-10-12 S. Heinemeyer , M. Mondragon , G. Zoupanos

I give an introductory review of recent, fascinating developments in supersymmetric gauge theories. I explain pedagogically the miraculous properties of supersymmetric gauge dynamics allowing one to obtain exact solutions in many instances.…

High Energy Physics - Theory · Physics 2011-04-15 M. Shifman

We analyse quantum properties of ${\cal N}=2$ and ${\cal N}=4$ supersymmetric gauge theories formulated in terms of ${\cal N}=1$ superfields and investigate the conditions imposed on a renormalization prescription under which the…

High Energy Physics - Theory · Physics 2023-05-24 Sergei Aleshin , Konstantin Stepanyantz

We consider a one-loop finite ${\cal N}=1$ supersymmetric theory in such a renormalization scheme that the first $L$ contributions to the gauge $\beta$-function and the first $(L-1)$ contributions to the anomalous dimension of the matter…

High Energy Physics - Theory · Physics 2021-07-12 Konstantin Stepanyantz

We study the possibility of an ultraviolet (UV) zero in the $n$-loop beta function of U(1) and non-Abelian gauge theories with $N_f$ fermions for large $N_f$. The effect of scheme transformations on the coefficients of different powers of…

High Energy Physics - Theory · Physics 2014-03-25 Robert Shrock

We extend to larger unification groups an earlier study exploring the possibility of unification of gauge symmetries in theories with dynamical symmetry breaking. Based on our results, we comment on the outlook for models that seek to…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ning Chen , Robert Shrock

The finiteness properties of the N=4 supersymmetric Yang-Mills theory are reanalyzed both in the component formulation and using N=1 superfields, in order to discuss some subtleties that emerge in the computation of gauge dependent…

High Energy Physics - Theory · Physics 2009-10-31 Stefano Kovacs

We investigate a supersymmetric theory with an extra U(1) gauge symmetry surviving down to low energies. The extra U(1) is assumed to originate from an E$_6$ grand unified theory (GUT). We show that if one assumes universal soft…

High Energy Physics - Phenomenology · Physics 2009-10-28 E. Keith , Ernest Ma , Biswarup Mukhopadhyaya

We review recent activity in the construction of the renormalization group functions for O(N) scalar and gauge theories in six and higher dimensions. The theories lie in their respective universality classes at the Wilson-Fisher fixed…

High Energy Physics - Theory · Physics 2016-10-17 J. A. Gracey

We establish the ultra-violet finiteness of various classes of noncommutative gauge theories.

High Energy Physics - Theory · Physics 2009-11-07 I. Jack , D. R. T. Jones

Manifestly invariant renormalization scheme for supersymmetric gauge theories is proposed. This scheme is applied to supersymmetric quantum electrodynamics.

High Energy Physics - Theory · Physics 2007-05-23 A. A. Slavnov , K. V. Stepanyantz

By considering the constraints from nucleon decay we obtain upper limits on tan beta in generalized supersymmetric SU(5) grand unified theories with gauge-mediated supersymmetry breaking. We find that the predicted values of tan beta in…

High Energy Physics - Phenomenology · Physics 2009-10-31 H. Hamidian , K. Huitu , K. Puolamaki , D. -X. Zhang

Recent developments in supersymmetric unified theories are reviewed, with particular emphasis on supersymmetric grand unification and a brief discussion of recent ideas about extra dimensions.

High Energy Physics - Phenomenology · Physics 2007-05-23 R. N. Mohapatra

Five-dimensional $\mathcal{N}=1$ theories with gauge group $U(N)$, $SU(N)$, $USp(2N)$ and $SO(N)$ are studied at large rank through localization on a large sphere. The phase diagram of theories with fundamental hypermultiplets is universal…

High Energy Physics - Theory · Physics 2021-07-19 Leonardo Santilli

We discuss questions related to renormalization group and to nonperturbative aspects of non-Abelian gauge theories with N=2 and/or N=1 supersymmetry. Results on perturbative and nonperturbative $\beta$ functions of these theories are…

High Energy Physics - Theory · Physics 2009-10-31 K. Konishi