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Related papers: On S-duality for Non-Simply-Laced Gauge Groups

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Characters of $E_8\otimes E_8$ and SO(32) heterotic strings involving the full internal symmetry Cartan subalgebra generators are defined after circle compactification so that they are T dual. The novel point, as compared with an earlier…

High Energy Physics - Theory · Physics 2009-10-31 Jean-Loup Gervais

We describe a new kind of transition between topologically distinct $N=2$ type II Calabi--Yau vacua through points with enhanced non-abelian gauge symmetries together with fundamental charged matter hypermultiplets. We connect the…

High Energy Physics - Theory · Physics 2009-10-30 P. Berglund , S. Katz , A. Klemm , P. Mayr

In heterotic string theory compactified on T^6, the T-duality orbits of dyons of charge (Q,P) are characterized by O(6,22;R) invariants Q^2, P^2 and Q.P together with a set of invariants of the discrete T-duality group O(6,22;Z). We study…

High Energy Physics - Theory · Physics 2009-09-15 Shamik Banerjee , Ashoke Sen

The moduli space of k G-instantons on R^4 for a classical gauge group G is known to be given by the Higgs branch of a supersymmetric gauge theory that lives on Dp branes probing D(p + 4) branes in Type II theories. For p = 3, these (3 + 1)…

High Energy Physics - Theory · Physics 2015-03-17 Sergio Benvenuti , Amihay Hanany , Noppadol Mekareeya

We propose an electric-magnetic duality and conjecture an exact conformal window for a class of non-supersymmetric U(N_c) gauge theories with fermions in the (anti)symmetric representation of the gauge group and N_f additional scalar and…

High Energy Physics - Theory · Physics 2008-11-26 Adi Armoni , Dan Israel , Gregory Moraitis , Vasilis Niarchos

We consider the S-duality transformation of gauge invariant operators and states in $\mathcal{N}$ $=4$ SYM theory. The transformation is realized through an operator $ S $ which is the $ SL(2,Z) $ canonical transformation in loop space with…

High Energy Physics - Theory · Physics 2019-05-23 Shan Hu

In discussions of the T-duality between the two heterotic string theories, the duality is actually implemented through the "common" SO(16) x SO(16) subgroup of "SO(32)" and E_8 x E_8. In fact, however, a global investigation shows that no…

High Energy Physics - Theory · Physics 2008-11-26 Brett McInnes

We survey some of the AGT relations between N=2 gauge theories in four dimensions and geometric representations of symmetry algebras of two-dimensional conformal field theory on the equivariant cohomology of their instanton moduli spaces.…

High Energy Physics - Theory · Physics 2016-10-12 Richard J. Szabo

Motivated by the recent work of Aubert-Xu and the techniques in G. Muic's article, we provide examples of computations of the Aubert-Zelevinsky duality functor for the principal and mediate series of the exceptional group $G_2$, and deduce…

Representation Theory · Mathematics 2025-05-26 Chuan Qin

The low energy structures of N=1 supersymmetric models with E_6, F_4 and E_7 gauge groups and fundamental irrep matter contents are studied herein. We identify sets of gauge invariant composites which label all flat directions in the…

High Energy Physics - Theory · Physics 2009-10-30 Peter Cho

The equations of motion of the massless sector of the two dimensional string theory, obtained by compactifying the heterotic string theory on an eight dimensional torus, is known to have an affine o(8,24) symmetry algebra generating an…

High Energy Physics - Theory · Physics 2016-09-06 Ashoke Sen

Toric Duality arises as an ambiguity in computing the quiver gauge theory living on a D3-brane which probes a toric singularity. It is reviewed how, in simple cases Toric Duality is Seiberg Duality. The set of all Seiberg Dualities on a…

High Energy Physics - Theory · Physics 2009-11-07 Sebastian Franco , Amihay Hanany

We examine several aspects of S-duality of four-dimensional noncommutative gauge theory. By making duality transformation explicit, we find that S-dual of noncommutative gauge theory is defined in terms of dual noncommutative deformation.…

High Energy Physics - Theory · Physics 2009-10-31 Soo-Jong Rey , Rikard von Unge

We study a class of four-dimensional N=1 heterotic string theories which have nontrivial quantum dynamics arising from asymptotically free gauge groups. These models are obtained by orbifolding 4d N=2 heterotic/type II dual pairs by…

High Energy Physics - Theory · Physics 2009-10-07 S. Kachru , E. Silverstein

For heterotic string theory compactified on T^6, we derive the complete set of T-duality invariants which characterize a pair of charge vectors (Q,P) labelling the electric and magnetic charges of the dyon. Using this we can identify the…

High Energy Physics - Theory · Physics 2009-09-15 Shamik Banerjee , Ashoke Sen

In this work the exceptional field theory formulation of supergravity with SL(5) gauge group is considered. This group appears as a U-duality group of $D=7$ maximal supergravity. In the formalism presented the hidden global duality group is…

High Energy Physics - Theory · Physics 2016-03-23 Edvard T. Musaev

The prepotential of N=2* supersymmetric theories with unitary gauge groups in an Omega-background satisfies a modular anomaly equation that can be recursively solved order by order in an expansion for small mass. By requiring that S-duality…

High Energy Physics - Theory · Physics 2015-10-23 M. Billo , M. Frau , F. Fucito , A. Lerda , J. F. Morales

We address non-perturbative effects and duality symmetries in $N=2$ heterotic string theories in four dimensions. Specifically, we consider how each of the four lines of enhanced gauge symmetries in the perturbative moduli space of $N=2$…

High Energy Physics - Theory · Physics 2016-08-15 Gabriel Lopes Cardoso , Dieter Lüst , Thomas Mohaupt

We study supersymmetric Sp(2N) gauge theories with matter in the antisymmetric tensor representation and F fundamentals. For F=6 we solve the theory exactly in terms of confined degrees of freedom and a superpotential. By adding mass terms…

High Energy Physics - Theory · Physics 2009-09-17 Csaba Csaki , Witold Skiba , Martin Schmaltz

We use localization techniques to study the non-perturbative properties of an N=2 superconformal gauge theory with gauge group SU(3) and six fundamental flavours. The instanton corrections to the prepotential, the dual periods and the…

High Energy Physics - Theory · Physics 2015-09-02 S. K. Ashok , M. Billó , E. Dell'Aquila , M. Frau , A. Lerda , M. Raman