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Related papers: Probing F-theory With Multiple Branes

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We calculate classical cross sections for absorption of massless scalars by the extremal 3-branes of type IIB theory, and by the extremal 2- and 5-branes of M-theory. The results are compared with corresponding calculations in the world…

High Energy Physics - Theory · Physics 2009-10-30 Igor R. Klebanov

While M- and F-theory compactifications describe a much larger class of vacua than perturbative string compactifications, they typically need singularities to generate non-abelian gauge fields and charged matter. The physical explanation…

High Energy Physics - Theory · Physics 2023-10-10 R. Donagi , M. Wijnholt

We determine all D-branes in the non-tachyonic 0'B orientifold, examine their world-volume anomalies and study orbifold compactifications. We find that the spectrum of the D-branes contains chiral fermions in the symmetric, antisymmetric…

High Energy Physics - Theory · Physics 2010-11-19 E. Dudas , J. Mourad

F-theory requires a new Virasoro algebra, including $\kappa$-symmetry, with a worldvolume coordinate for each generator. (Similar is implied for the superstring.) Doubles of the spacetime coordinates are eliminated by selfduality, which now…

High Energy Physics - Theory · Physics 2017-11-16 William Linch , Warren Siegel

We consider p-branes with one or more circular directions fibered over the transverse space. The fibration, in conjunction with the transverse space having a blown-up cycle, enables these p-brane solutions to be completely regular. Some…

High Energy Physics - Theory · Physics 2014-12-30 Justin F. Vazquez-Poritz , Zhibai Zhang

We construct a black hole geometry dual to a (2+1)-dimensional defect in an ambient (3+1)-dimensional gauge theory at non-zero temperature and quark density. The geometry is a solution to the equations of motion of type IIB supergravity…

High Energy Physics - Theory · Physics 2022-10-26 Ana Garbayo , Carlos Hoyos , Niko Jokela , José Manuel Penín , Alfonso V. Ramallo

We discuss some aspects of the relation between space-time properties of branes in string theory, and the gauge theory on their worldvolume, for models invariant under four supercharges in three and four dimensions. We show that a simple…

High Energy Physics - Theory · Physics 2009-10-30 S. Elitzur , A. Giveon , D. Kutasov , E. Rabinovici , A. Schwimmer

We construct two-dimensional N=(2,2) supersymmetric gauge theories with orthogonal and symplectic groups using branes and orientifold planes in Type IIA string theory. A number of puzzles regarding the construction, including the effect of…

High Energy Physics - Theory · Physics 2018-08-29 Oren Bergman , Eran Avraham

We review and extend the progress made over the past few years in understanding the structure of toric quiver gauge theories; those which are induced on the world-volume of a stack of D3-branes placed at the tip of a toric Calabi-Yau cone,…

High Energy Physics - Theory · Physics 2008-11-26 Kristian D. Kennaway

We construct supersymmetric M3-brane solutions in D=11 supergravity. They can be viewed as deformations of backgrounds taking the form of a direct product of four-dimensional Minkowski spacetime and a non-compact Ricci-flat manifold of G_2…

High Energy Physics - Theory · Physics 2009-09-17 M. Cvetic , H. Lu , C. N. Pope

Three-dimensional conformal field theories (CFTs) of deconfined gauge fields coupled to gapless flavors of fermionic and bosonic matter describe quantum critical points of condensed matter systems in two spatial dimensions. An important…

High Energy Physics - Theory · Physics 2012-05-15 Igor R. Klebanov , Silviu S. Pufu , Subir Sachdev , Benjamin R. Safdi

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

Six dimensional bulk spacetimes with 3-- and 4--branes are constructed using certain non--conventional bulk scalars as sources. In particular, we investigate the consequences of having the phantom (negative kinetic energy) and the…

High Energy Physics - Theory · Physics 2009-11-11 Ratna Koley , Sayan Kar

We consider M theory 5-branes with compact transverse dimensions. In certain limits the theory on the 5-brane decouples and defines ``little string theories'' in 5+1 dimensions. We show that the familiar structure of IIA/IIB,M,F- theory in…

High Energy Physics - Theory · Physics 2016-09-06 Andrei Losev , Gregory Moore , Samson L. Shatashvili

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 derive D-brane gauge theories for C^3/Z_n x Z_n orbifolds with discrete torsion and study the moduli space of a D-brane at a point. We show that, as suggested in previous work, closed string moduli do not fully resolve the singularity,…

High Energy Physics - Theory · Physics 2009-10-31 Michael R. Douglas , Bartomeu Fiol

We compute the quantum fluctuations of a 3-brane with tension, energy density and stiffness. As a result of the fluctuations there are induced forces between massive objects living on the brane. We study various limiting cases of the…

High Energy Physics - Theory · Physics 2007-05-23 Bayram Tekin

We study D1-branes on the fourfold $\C^4/(\Z_2\times\Z_2\times\Z_2)$, in the presence of discrete torsion. Discrete torsion is incorporated in the gauge theory of the D1-branes by considering a projective representation of the finite group…

High Energy Physics - Theory · Physics 2009-10-31 Subir Mukhopadhyay , Koushik Ray

We argue that the moduli space for the Bagger-Lambert A_4 theory at level k is (R^8 \times R^8)/D_{2k}, where D_{2k} is the dihedral group of order 4k. We conjecture that the theory describes two M2-branes on a Z_{2k} ``M-fold'', in which a…

High Energy Physics - Theory · Physics 2009-12-04 Jacques Distler , Sunil Mukhi , Constantinos Papageorgakis , Mark Van Raamsdonk

By analyzing $F$-theory on $K3$ near the orbifold limit of $K3$ we establish the equivalence between $F$-theory on $K3$ and an orientifold of type IIB on $T^2$, which in turn, is related by a T-duality transformation to type I theory on…

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