We examine N=1 supersymmetric gauge theories which confine in the presence of a tree-level superpotential. We show the confining spectra which satisfy the 't Hooft anomaly matching conditions and give a simple method to find the confining superpotential. Using this method we fix the confining superpotentials in the simplest cases, and show how these superpotentials are generated by multi-instanton effects in the dual theory. These new type of confining theories may be useful for model building, since the size of the matter content is not restricted by an index constraint. Therefore, one expects that a large variety of new confining spectra can be obtained using such models
The fivebrane of M theory is used in order to study the moduli space of vacua of confining phase N=1...
We give a brief account of the recent progresses in super Yang-Mills theories based in particular on...
The fivebrane of M theory is used in order to study the moduli space of vacua of confining phase N=1...
We examine N=1 supersymmetric gauge theories which confine in the presence of a tree-level superpote...
The authors give a classification and overview of the confining N = 1 supersymmetric gauge theories....
Abstract We propose a new set of s-confining theories with product gauge groups and no tree-level su...
Abstract We propose new classes of 4d N $$ \mathcal{N} $$ = 1 S-confining gauge theories, with a sim...
In this thesis we review the Seiberg-Witten solution of four dimensional N=2 gauge theories, the six...
We consider four dimensional $\mathcal{N}=1$ gauge theories that are S-confining, that is they are d...
We give necessary criteria for N=1 supersymmetric theories to be in a smoothly confining phase witho...
It has been known that the fivebrane of type IIA theory can be used to give an exact low energy desc...
Abstract In this work we present a new class of N $$ \mathcal{N} $$ = 1 supersymmetric confining gau...
AbstractIn this Letter we consider models with N U(1) gauge fields Aμn together with N Kalb–Ramond f...
We study the confining phase structure on {\cal N}=1 supersymmetric SO(12) gauge theory with N_f \le...
Abelian theories in three dimensions can have linearly confining phases as a result of monopole-inst...
The fivebrane of M theory is used in order to study the moduli space of vacua of confining phase N=1...
We give a brief account of the recent progresses in super Yang-Mills theories based in particular on...
The fivebrane of M theory is used in order to study the moduli space of vacua of confining phase N=1...
We examine N=1 supersymmetric gauge theories which confine in the presence of a tree-level superpote...
The authors give a classification and overview of the confining N = 1 supersymmetric gauge theories....
Abstract We propose a new set of s-confining theories with product gauge groups and no tree-level su...
Abstract We propose new classes of 4d N $$ \mathcal{N} $$ = 1 S-confining gauge theories, with a sim...
In this thesis we review the Seiberg-Witten solution of four dimensional N=2 gauge theories, the six...
We consider four dimensional $\mathcal{N}=1$ gauge theories that are S-confining, that is they are d...
We give necessary criteria for N=1 supersymmetric theories to be in a smoothly confining phase witho...
It has been known that the fivebrane of type IIA theory can be used to give an exact low energy desc...
Abstract In this work we present a new class of N $$ \mathcal{N} $$ = 1 supersymmetric confining gau...
AbstractIn this Letter we consider models with N U(1) gauge fields Aμn together with N Kalb–Ramond f...
We study the confining phase structure on {\cal N}=1 supersymmetric SO(12) gauge theory with N_f \le...
Abelian theories in three dimensions can have linearly confining phases as a result of monopole-inst...
The fivebrane of M theory is used in order to study the moduli space of vacua of confining phase N=1...
We give a brief account of the recent progresses in super Yang-Mills theories based in particular on...
The fivebrane of M theory is used in order to study the moduli space of vacua of confining phase N=1...