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Related papers: On Three Dimensional Quiver Gauge Theories and Int…

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We propose a deformation principle of gauge theories in three dimensions that can describe topologically stable self-dual gauge fields, i.e., vacua configurations that in spite of their masses do not deform the background geometry and are…

High Energy Physics - Theory · Physics 2015-06-19 Julio Oliva , Mauricio Valenzuela

We present an exact description of the metric on the moduli space of vacua and the spectrum of massive states for four dimensional N=2 supersymmetric SU(n) gauge theories. The moduli space of quantum vacua is identified with the moduli…

High Energy Physics - Theory · Physics 2009-10-28 Philip C. Argyres , Alon E. Faraggi

We construct and analyze dual N=4 supersymmetric gauge theories in three dimensions with unitary and symplectic gauge groups. The gauge groups and the field content of the theories are encoded in quiver diagrams. The duality exchanges the…

High Energy Physics - Theory · Physics 2009-09-17 Jan de Boer , Kentaro Hori , Hirosi Ooguri , Yaron Oz

Seiberg-Witten geometry of mass deformed $\mathcal N=2$ superconformal ADE quiver gauge theories in four dimensions is determined. We solve the limit shape equations derived from the gauge theory and identify the space $\mathfrak M$ of…

High Energy Physics - Theory · Physics 2023-07-21 Nikita Nekrasov , Vasily Pestun

We prove a duality, recently conjectured in arXiv:1103.5726, which relates the F-terms of supersymmetric gauge theories defined in two and four dimensions respectively. The proof proceeds by a saddle point analysis of the four-dimensional…

High Energy Physics - Theory · Physics 2011-09-13 Heng-Yu Chen , Nick Dorey , Timothy J. Hollowood , Sungjay Lee

We study marginal and relevant supersymmetric deformations of the N=4 super-Yang-Mills theory in four dimensions. Our primary innovation is the interpretation of the moduli spaces of vacua of these theories as non-commutative spaces. The…

High Energy Physics - Theory · Physics 2009-10-31 David Berenstein , Vishnu Jejjala , Robert G. Leigh

We consider four-dimensional N=2 supersymmetric gauge theories with gauge group U(N) on R^3 x S^1, in the presence of a classical superpotential. The low-energy quantum superpotential is obtained by simply replacing the adjoint scalar…

High Energy Physics - Theory · Physics 2010-12-03 Rutger Boels , Jan de Boer , Robert Duivenvoorden , Jeroen Wijnhout

We consider the vacuum structure of the finite N=2 theory with N_f=2N fundamental hypermultiplets broken to N=1 by a superpotential for the adjoint chiral multiplet. We do this in two ways: firstly, by compactification to three dimensions,…

High Energy Physics - Theory · Physics 2010-12-03 Timothy J. Hollowood , Kazutoshi Ohta

We construct a four dimensional Yang-Mills theory with ${\cal N}=4$ twisted supersymmetry whose classical vacua correspond to four dimensional anti-de Sitter space. The theory utilizes a complex gauge field whose real part is a spin…

High Energy Physics - Theory · Physics 2009-01-07 Simon Catterall

We consider compactifications of type IIA superstring theory on mirror-folds obtained as K3 fibrations over two-tori with non-geometric monodromies involving mirror symmetries. At special points in the moduli space these are asymmetric…

High Energy Physics - Theory · Physics 2018-10-16 Chris Hull , Dan Israel , Alessandra Sarti

We consider generic properties of the moduli space of vacua in $N=2$ supersymmetric Yang--Mills theory recently studied by Seiberg and Witten. We find, on general grounds, Picard--Fuchs type of differential equations expressing the…

High Energy Physics - Theory · Physics 2017-09-07 A. Ceresole , R. D'Auria , S. Ferrara

We consider the compactifcation of 5d non-simply laced fractional quiver gauge theory constructed in arXiv:1705.04410. In contrast to the simply laced quivers, here two $\Omega$-background parameters play different roles, so that we can…

High Energy Physics - Theory · Physics 2018-07-12 Heng-Yu Chen , Taro Kimura

We found a lot of new three dimensional N = 4 mirror pairs generalizing previous considerations on three dimensional generalized quiver gauge theories. We recovered almost all previous discovered mirror pairs with these constructions. One…

High Energy Physics - Theory · Physics 2011-05-23 Dimitri Nanopoulos , Dan Xie

We discuss the mass-deformed N=4 SU(N) supersymmetric Yang-Mills theory (also known as the N=1* theory). We analyze how the correlation functions of this theory transform under S-duality, and which correlation functions depend…

High Energy Physics - Theory · Physics 2009-10-31 Ofer Aharony , Nick Dorey , S. Prem Kumar

Extending previous work on geometric engineering of N=1 Yang-Mills in four dimensions for simply laced ($A_n,D_n,E_{6,7,8}$) gauge groups, we construct local models for all other gauge groups ($B_n,C_n,F_4,G_2$) in terms of F-theory. We…

High Energy Physics - Theory · Physics 2008-11-26 Cumrun Vafa

We realize four-dimensional N=2 superconformal quiver gauge theories with alternating SO and USp gauge groups as compactifications of the six-dimensional D_N theory with defects. The construction can be used to analyze infinitely…

High Energy Physics - Theory · Physics 2009-08-06 Yuji Tachikawa

We present a comprehensive classification of supersymmetric vacua of M-theory compactification on seven-dimensional manifolds with general four-form fluxes. We analyze the cases where the resulting four-dimensional vacua have N = 1,2,3,4…

High Energy Physics - Theory · Physics 2008-11-26 Klaus Behrndt , Mirjam Cvetic , Tao Liu

General string-theoretic considerations suggest that four-dimensional large-N gauge theories should have dual descriptions in terms of two-dimensional conformal field theories. However, for non-supersymmetric confining theories such as pure…

High Energy Physics - Theory · Physics 2015-11-25 Gokce Basar , Aleksey Cherman , Keith R. Dienes , David A. McGady

We show how the Dijkgraaf-Vafa matrix model proposal can be extended to describe five-dimensional gauge theories compactified on a circle to four dimensions. This involves solving a certain quantum mechanical matrix model. We do this for…

High Energy Physics - Theory · Physics 2010-11-19 Timothy J. Hollowood

Spatial compactification on $\mathbb R^{3} \times \mathbb S^1_L$ at small $\mathbb S^1$-size $L$ often leads to a calculable vacuum structure, where various "topological molecules" are responsible for confinement and the realization of the…

High Energy Physics - Theory · Physics 2015-09-25 Mohamed M. Anber , Erich Poppitz