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Brane Box Models of intersecting NS and D5 branes are mapped to D3 branes at C^3/Gamma orbifold singularities and vise versa, in a setup which gives rise to N=1 supersymmetric gauge theories in four dimensions. The Brane Box Models are…

High Energy Physics - Theory · Physics 2010-04-06 Amihay Hanany , Angel M. Uranga

U-duality symmetry of M-theory and S and T-duality of string theory can be used to study various black branes solutions. We explore some aspect of this idea here. This symmetry can be used to get relations among various components of the…

High Energy Physics - Theory · Physics 2015-12-23 Samrat Bhowmick

Just as D-brane charge of Type IIA and Type IIB superstrings is classified, respectively, by K^1(X) and K(X), Ramond-Ramond fields in these theories are classified, respectively, by K(X) and K^1(X). By analyzing a recent proposal for how to…

High Energy Physics - Theory · Physics 2010-04-07 Gregory Moore , Edward Witten

We discuss string theory relations between gravity and gauge theory tree amplitudes. Together with $D$-dimensional unitarity, these relations can be used to perturbatively quantize gravity theories, i.e. they contain the necessary…

High Energy Physics - Theory · Physics 2007-05-23 Z. Bern

We show that the singular sources in the energy-momentum tensor for the Randall-Sundrum brane world, viewed as a solution of type IIB supergravity, are composed of two elements. One of these is a D3-brane source with tension opposite in…

High Energy Physics - Theory · Physics 2009-09-17 M. Cvetic , M. J. Duff , James T. Liu , H. Lu , C. N. Pope , K. S. Stelle

Recent studies of scattering amplitudes in planar N=4 SYM theory revealed the existence of a hidden dual superconformal symmetry. Together with the conventional superconformal symmetry it gives rise to powerful restrictions on the planar…

High Energy Physics - Theory · Physics 2014-11-20 G. P. Korchemsky , E. Sokatchev

The six gluon disk amplitude is calculated in superstring theory. This amplitude probes the gauge interactions with six external legs on Dp-branes, in particular including e.g. F^6-terms. The full string S-matrix can be expressed by six…

High Energy Physics - Theory · Physics 2007-05-23 D. Oprisa , S. Stieberger

In the name of supersymmetric double field theory, superstring effective actions can be reformulated into simple forms. They feature a pair of vielbeins corresponding to the same spacetime metric, and hence enjoy double local Lorentz…

High Energy Physics - Theory · Physics 2012-09-28 Imtak Jeon , Kanghoon Lee , Jeong-Hyuck Park

This thesis deals with the two duality symmetries of N=2 D=10 supergravity theories that are descendant from the full superstring theory: fermionic T-duality and U-duality. The fermionic T-duality transformation is applied to the D-brane…

High Energy Physics - Theory · Physics 2012-01-04 Ilya Bakhmatov

We classify the half-supersymmetric "domain walls", i.e. branes of codimension one, in toroidally compactified IIA/IIB string theory and show to which gauged supergravity theory each of these domain walls belong. We use as input the…

High Energy Physics - Theory · Physics 2013-05-30 Eric A. Bergshoeff , Axel Kleinschmidt , Fabio Riccioni

As was shown in arXiv:1203.1054, expanding the Nambu action near the "long string" vacuum in the static gauge one finds that the one-loop 2 to 2 scattering amplitude of the $D-2=24$ transverse 2d fluctuations $X^i$ is given by a pure phase…

High Energy Physics - Theory · Physics 2025-08-06 Arkady A. Tseytlin , Zihan Wang

The bracket operation on mutually local BRST classes may be combined with Lorentz invariance and analyticity to write an infinite set of finite difference relations on string scattering amplitudes. When combined with some simple physical…

High Energy Physics - Theory · Physics 2008-02-03 Gregory Moore

This thesis is devoted to various questions connected with duality. It is composed of two parts. The first part discusses some aspects of timelike T-duality. We explore the possibility of compactification of supergravity theories with…

High Energy Physics - Theory · Physics 2018-10-08 Arash Ranjbar

Gravitational corrections in N=1 and N=2 supersymmetric gauge theories are obtained from topological string amplitudes. We show how they are recovered in matrix model computations. This provides a test of the proposal by Dijkgraaf and Vafa…

High Energy Physics - Theory · Physics 2010-04-06 Albrecht Klemm , Marcos Marino , Stefan Theisen

We construct supergravity plus branes solutions, which we argue to be related to 4d N=1 SQCD with a quartic superpotential. The geometries depend on the ratio Nf/Nc which can be kept of order one, present a good singularity at the origin…

High Energy Physics - Theory · Physics 2010-04-06 Roberto Casero , Carlos Nunez , Angel Paredes

We consider compactifications of the matrix model of M-theory on $S^1/Z_2\times T^d$ for $d>0$, and interpret them as orbifolds of the supersymmetric U(N) Yang-Mills theory on $R\times T^{d+1}$. The orbifold group acts both on the gauge…

High Energy Physics - Theory · Physics 2016-09-06 Petr Horava

Extending recent work on SU gauge theory, we engineer local string models for N=1 four-dimensional SO and USp gauge theories coupled to matter in the fundamental. The local models are type IIB orientifolds with D7 branes on a curved…

High Energy Physics - Theory · Physics 2016-09-06 Cumrun Vafa , Barton Zwiebach

Working within a five-dimensional consistent truncation of type IIB supergravity dimensionally reduced on $T^{1,1}$, we consider supersymmetry breaking solutions with the asymptotics of the supersymmetric Klebanov-Strassler background.…

High Energy Physics - Theory · Physics 2015-11-30 Matteo Bertolini , Daniele Musso , Ioannis Papadimitriou , Himanshu Raj

We explore two different problems in string theory in which duality relates an ordinary p-form in one theory to a self-dual (p+1)-form in another theory. One problem involves comparing D4-branes to M5-branes, and the other involves…

High Energy Physics - Theory · Physics 2010-04-07 Edward Witten

We work out Seiberg-like dualities for 3d $\mathcal{N}=2$ theories with SU(N) gauge group. We use the $SL(2,\mathbb{Z})$ action on 3d conformal field theories with U(1) global symmetry. One of generator S of $SL(2,\mathbb{Z})$ acts as…

High Energy Physics - Theory · Physics 2017-09-07 Jaemo Park , Kyung-Jae Park
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