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We consider compactifications of the N=1, d=6, E_8 theory on tori to five, four, and three dimensions and learn about some properties of this theory. As a by-product we derive the SL(2,\IZ) duality of the N=2, d=4, SU(2) theory with N_f=4.…

High Energy Physics - Theory · Physics 2009-09-15 Ori J. Ganor , David R. Morrison , Nathan Seiberg

Dvali and Shifman have proposed a field-theoretic mechanism for localizing gauge fields to "branes" in higher dimensional spaces using confinement in a bulk gauge theory. The resulting objects have a number of qualitative features in common…

High Energy Physics - Theory · Physics 2009-10-31 Nima Arkani-Hamed , Martin Schmaltz

In the context of low-energy effective theory of multiple M2-branes, we construct the interaction terms between the world-volume fields of M2-branes and the antisymmetric tensor fields of three- and six-forms. By utilizing the…

High Energy Physics - Theory · Physics 2015-05-13 Yoonbai Kim , O-Kab Kwon , Hiroaki Nakajima , D. D. Tolla

We consider the type I theory compactified on $T^3$. When the D5-brane wraps the $T^3$ it yields a D2-brane in seven dimensions. In the leading approximation the moduli space of vacua of the three dimensional field theory on the brane is…

High Energy Physics - Theory · Physics 2009-09-15 Nathan Seiberg

We study compactifications of string theory and M-theory to six dimensions with background fluxes. The nonzero fluxes lead to additional mass parameters. We derive the S- and T-duality rules for the corresponding (massive) supergravity…

High Energy Physics - Theory · Physics 2008-12-18 K. Behrndt , E. Bergshoeff , D. Roest , P. Sundell

We analyze how string theory dualities may be described in M theory. T dualities arise from scalar-vector dualities in the worldvolume of the membrane of M theory. ``Electric-magnetic'' dualities arise from a duality transformation in M…

High Energy Physics - Theory · Physics 2009-09-29 Ofer Aharony

We argue that all conjectured dualities involving various string, M- and F- theory compactifications can be `derived' from the conjectured duality between type I and SO(32) heterotic string theory, T-dualities, and the definition of M- and…

High Energy Physics - Theory · Physics 2009-09-15 Ashoke Sen

We give a unified description of all BPS states of M-theory compactified on $T^5$ in terms of the five-brane. We compute the mass spectrum and degeneracies and find that the $SO(5,5,Z)$ U-duality symmetry naturally arises as a T-duality by…

High Energy Physics - Theory · Physics 2009-07-09 R. Dijkgraaf , E. Verlinde , H. Verlinde

In addition to being a prime candidate for a fundamental unified theory of all interactions in nature, string theory provides a natural setting to understand gauge field theories. This is linked to the concept of "D-branes": extended,…

High Energy Physics - Phenomenology · Physics 2015-06-25 Sunil Mukhi

Three subjects are considered here: a self-dual non-critical string that appears in Type IIB superstring theory at points in ${\rm K3}$ moduli space where the Type IIA theory has extended gauge symmetry; a conformal field theory singularity…

High Energy Physics - Theory · Physics 2007-05-23 Edward Witten

We describe a class of six-dimensional conformal field theories that have some properties in common with and possibly are related to a subsector of the tensionless string theories. The latter theories can for example give rise to…

High Energy Physics - Theory · Physics 2009-10-31 Mans Henningson

We study electric-magnetic duality in compactifications of M-theory on twisted connected sum (TCS) $G_2$ manifolds via duality with F-theory. Specifically, we study the physics of the D3-branes in F-theory compactified on a Calabi-Yau…

High Energy Physics - Theory · Physics 2023-05-10 James Halverson , Benjamin Sung , Jiahua Tian

The (2,2) world-sheet supersymmetric string theory is discussed from the viewpoint of string/membrane unification. The effective field theory in the closed string target space is known to be the 2+2 dimensional (integrable) theory of…

High Energy Physics - Theory · Physics 2007-05-23 Sergei V. Ketov

We suggest that the (2,0) six dimensional field theory compactified on $S^1\times K3$ is the Matrix model description of both M-theory on $K3$ and the Heterotic string on $T^3$. This proposal is different from existing proposals for the…

High Energy Physics - Theory · Physics 2009-10-30 Micha Berkooz , Moshe Rozali

A fully realistic and systematic effective field theory model of a 3-brane universe is constructed. It consists of a six-dimensional gravitating spacetime, containing several, approximately parallel (3+1)-dimensional defects, or…

High Energy Physics - Phenomenology · Physics 2009-09-15 Raman Sundrum

In these lectures, two different aspects of brane world scenarios in 5d gravity or string theory are discussed. In the first two lectures, work on how warped compactifications of 5d gravity theories can change the guise of the hierarchy…

High Energy Physics - Theory · Physics 2017-08-23 S. Kachru

A duality relationship between certain brane configurations in type IIA and type IIB string theory is explored by exploiting the geometrical origins of each theory in M-theory. The configurations are dual ways of realising the…

High Energy Physics - Theory · Physics 2009-10-30 Clifford V. Johnson

We study supersymmetric embeddings of D-brane probes of different dimensionality in the AdS_5xL^{abc} background of type IIB string theory. In the case of D3-branes, we recover the known three-cycles dual to the dibaryonic operators of the…

High Energy Physics - Theory · Physics 2009-11-11 Felipe Canoura , Jose D. Edelstein , Alfonso V. Ramallo

A particular two-parameter class of little string theories can be described by $M$ parallel M5-branes probing a transverse affine $A_{N-1}$ singularity. We previously discussed the duality between the theories labelled by $(N,M)$ and…

High Energy Physics - Theory · Physics 2017-09-13 Stefan Hohenegger , Amer Iqbal , Soo-Jong Rey

We show that a set of parallel 3-brane probes near a conifold singularity can be mapped onto a configuration of intersecting branes in type IIA string theory. The field theory on the probes can be explicitly derived from this formulation.…

High Energy Physics - Theory · Physics 2008-11-26 Keshav Dasgupta , Sunil Mukhi