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Supersymmetric Sp(k) quantum chromodynamics with 8 supercharges in space-time dimensions 3 to 6 can be realised by two different Type II brane configurations in the presence of orientifolds. Consequently, two types of magnetic quivers…

High Energy Physics - Theory · Physics 2022-03-09 Satoshi Nawata , Marcus Sperling , Hao Ellery Wang , Zhenghao Zhong

In this article we study a family of four-dimensional, $\mathcal{N}=2$ supergravity theories that interpolates between all the single dilaton truncations of the $\mathrm{SO}(8)$ gauged $\mathcal{N}=8$ supergravity. In this infinitely many…

High Energy Physics - Theory · Physics 2021-04-09 Andres Anabalon , Dumitru Astefanesei , Antonio Gallerati , Mario Trigiante

A correspondence between type IIB string theory with N D7-branes on R^{1,3} x C^1/Z_2 x T^2/Z_2 x T^2/Z_2 and pure N=1 SU(N) gauge theory in four dimensions is proposed and argued. First the supergravity background of unwrapped and flat…

High Energy Physics - Theory · Physics 2013-05-29 Girma Hailu

String theory contains various extended objects. Among those, objects of codimension two (such as the D7-brane) are particularly interesting. Codimension two objects carry non-Abelian charges which are elements of a discrete U-duality group…

High Energy Physics - Theory · Physics 2014-11-19 Jan de Boer , Daniel R. Mayerson , Masaki Shigemori

We find a dual gravity theory to pure confining N=1 supersymmetric SU(N) gauge theory in four dimensions which has the correct gauge coupling running in addition to reproducing the appropriate pattern of chiral symmetry breaking. It is…

High Energy Physics - Theory · Physics 2008-01-03 Girma Hailu

We construct 3d, N=2 supersymmetric gauge theories by considering a one-parameter `R-flow' of 4d, N=2 theories, where the central charges vary while preserving their phase order. Each BPS state in 4d leads to a BPS particle in 3d, and thus…

High Energy Physics - Theory · Physics 2011-10-11 Sergio Cecotti , Clay Cordova , Cumrun Vafa

We consider the unification of gauge, Higgs as well as the matter fields in a 6D N=2 supersymmetric SU(8) gauge theory. The gauge symmetry SU(8) is broken down to SU(4) x SU(2)_L x SU(2)_R x U(1)^2 in 4D through T^2/Z_6 orbifold…

High Energy Physics - Phenomenology · Physics 2010-11-19 Ilia Gogoladze , Yukihiro Mimura , S. Nandi

We give a large class of supersymmetric domain walls in maximal seven-dimensional gauged supergravity with various types of gauge groups. Gaugings are described by components of the embedding tensor transforming in representations…

High Energy Physics - Theory · Physics 2019-08-27 Parinya Karndumri , Patharadanai Nuchino

We define the notion of a complete N=2 supersymmetric theory in 4 dimensions as a UV complete theory for which all the BPS central charges can be arbitrarily varied as we vary its Coulomb branch parameters, masses, and coupling constants.…

High Energy Physics - Theory · Physics 2013-04-12 Sergio Cecotti , Cumrun Vafa

The form of the most general orbifold breaking of gauge, global and supersymmetries with a single extra dimension is given. In certain theories the Higgs boson mass is ultraviolet finite due to an unbroken local supersymmetry, which is…

High Energy Physics - Theory · Physics 2010-05-28 Riccardo Barbieri , Lawrence J. Hall , Yasunori Nomura

We study the BPS spectrum of four-dimensional $\mathcal{N}=2$ superconformal field theory of Argyres-Douglas type, obtained via twisted compactification of six-dimensional $A_{N-1}$ $(2,0)$ theory on a sphere with an irregular puncture, by…

High Energy Physics - Theory · Physics 2013-12-24 Kazunobu Maruyoshi , Chan Y. Park , Wenbin Yan

This paper contains the results of our investigations of BPS instantons and of our work on N=2 supersymmetric gauge theories. The BPS instantons we study appear in type II string theory compactifications on Calabi-Yau threefolds. In the…

High Energy Physics - Theory · Physics 2007-08-10 Mathijs de Vroome

Starting from an N=1 supersymmetric electric gauge theory with the multiple product gauge group and the bifundamentals, we apply Seiberg dual to each gauge group, obtain the N=1 supersymmetric dual magnetic gauge theories with dual matters…

High Energy Physics - Theory · Physics 2009-11-05 Changhyun Ahn

We give a detailed discussion of the matching of the BPS states of heterotic, type I and type I' theories in d=9 for general backgrounds. This allows us to explicitly identify these (composite) brane states in the type I' theory that lead…

High Energy Physics - Theory · Physics 2009-10-30 D. Matalliotakis , H. P. Nilles , S. Theisen

We consider a one-dimensional Osp($N|2M$) pseudoparticle mechanical model which may be written as a phase space gauge theory. We show how the pseudoparticle model naturally encodes and explains the two-dimensional zero curvature approach to…

High Energy Physics - Theory · Physics 2009-10-22 Karyn M. Apfeldorf , Joaquim Gomis

Higher dimensional grand unified theories, with gauge symmetry breaking by orbifold compactification, possess SU(5) breaking at fixed points, and do not automatically lead to tree-level gauge coupling unification. A new framework is…

High Energy Physics - Phenomenology · Physics 2009-09-29 Lawrence J. Hall , Yasunori Nomura

We use the M theory approach in the presence of an orientifold O6 plane to understand some aspects of the moduli space of vacua for N=1 supersymmetric $SO(N_c)/Sp(N_c)$ gauge theories in four dimensions. By exploiting some general…

High Energy Physics - Theory · Physics 2016-08-25 Changhyun Ahn , Kyungho Oh , Radu Tatar

We systematically classify 1/2, 1/4 and 1/8 BPS equations in SUSY gauge theories in d=6, 5, 4, 3 and 2 with eight supercharges, with gauge groups and matter contents being arbitrary. Instantons (strings) and vortices (3-branes) are only…

High Energy Physics - Theory · Physics 2010-04-05 Minoru Eto , Youichi Isozumi , Muneto Nitta , Keisuke Ohashi

According to a recent classification of 6d (1,0) theories within F-theory there are only six "pure" 6d gauge theories which have a UV superconformal fixed point. The corresponding gauge groups are $SU(3),SO(8),F_4,E_6,E_7$, and $E_8$. These…

High Energy Physics - Theory · Physics 2017-10-25 Michele Del Zotto , Guglielmo Lockhart

We study four N=1 SU(N)^6 gauge theories, with bi-fundamental chiral matter and a superpotential. In the infrared, these gauge theories all realize the low-energy world-volume description of N coincident D3-branes transverse to the complex…

High Energy Physics - Theory · Physics 2011-10-11 C. E. Beasley , M. R. Plesser