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Related papers: Strings from Membranes and Fivebranes

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We discuss three classes of solitonic solutions in string theory: instantons, monopoles and string-like solitons. Instantons may provide a nonperturbative understanding of the vacuum structure of string theory, while monopoles may appear in…

High Energy Physics - Theory · Physics 2007-05-23 Ramzi R. Khuri

In view of the expectation that the solitonic sector of the lower dimensional world may be originated from the solitonic sector of string theory, various solitonic solutions are reduced from the heterotic fivebrane solutions in the…

High Energy Physics - Theory · Physics 2007-05-23 HoSeong La

It has been conjectured that Little String Theories in six dimensions are holographic to critical string theory in a linear dilaton background. We test this conjecture for theories arising on the worldvolume of heterotic fivebranes. We…

High Energy Physics - Theory · Physics 2009-10-31 Martin Gremm , Anton Kapustin

We give the general solution for the elementary and solitonic D-brane configurations as a result of a reinterpretation of the already known p-branes. These solutions are found by means of a relevant conformal transformation on the string…

High Energy Physics - Theory · Physics 2007-05-23 Pedro J. Silva

We apply the string-triality\cite{duffetal} to argue the existence of the string-networks of solitonic T and U-strings in the heterotic theory on T^6, S and T-strings in IIB on K3 x T^2 and, S and U-strings in IIA on K3 x T^2. We then show…

High Energy Physics - Theory · Physics 2010-02-03 Alok Kumar , Aalok Misra

Magnetic monopole solutions to heterotic string theory are discussed in toroidal compactifications to four spacetime dimensions. Particular emphasis is placed on the relation to previously studied fivebrane solutions in ten dimensions and…

High Energy Physics - Theory · Physics 2010-11-01 Jerome P. Gauntlett , Jeffrey A. Harvey , James T. Liu

We show that unstable D-branes play the role of ``D-sphalerons'' in string theory. Their existence implies that the configuration space of Type II string theory has a complicated homotopy structure, similar to that of an infinite…

High Energy Physics - Theory · Physics 2009-10-31 Jeffrey A. Harvey , Petr Horava , Per Kraus

A naive dimensional reduction of the $N=1, D=10$ supergravity theory that naturally arises in five-brane models is used to determine the r\^ole of two fields which are basic ingredients of string models: the dilaton and, among the moduli,…

High Energy Physics - Theory · Physics 2009-10-22 P. Binetruy

We discuss various dual {\it pairs} of $M$-theory compactifications. Each pair consists of a compactification in which the two-brane plays the crucial role in relation to a string theory and a compactification in which the five-brane takes…

High Energy Physics - Theory · Physics 2007-05-23 B. S. Acharya

We argue that M2 brane is realized as a topological soliton on a coincident pair of M5 and anti-M5 branes, as the two five-branes annihilate each other. Topology and quantum numbers of this world-volume soliton are discussed in some detail,…

High Energy Physics - Theory · Physics 2009-10-31 Piljin Yi

1. Preliminaries. 2. Heterotic string and motivations for large volume compactifications; 2.1 Gauge coupling unification; 2.2 Supersymmetry breaking by compactification. 3. M-theory on S^1/Z_2 \times Calabi-Yau. 4. Type I/I' string theory…

High Energy Physics - Theory · Physics 2007-05-23 I. Antoniadis

We compute the gravitational coupling $F_1$ for IIA string theory on $K3 \times T^2$ and use string-string duality to deduce the corresponding term for heterotic string on $T^6$. The latter is an infinite sum of gravitational instanton…

High Energy Physics - Theory · Physics 2016-08-25 Jeffrey A. Harvey , Gregory Moore

Matrix string theory is equivalent to type IIA superstring theory in the light-cone gauge, together with extra degrees of freedom representing D-brane states. It is therefore the appropriate framework in which to study systems of multiple…

High Energy Physics - Theory · Physics 2009-11-07 Dominic Brecher , Bert Janssen , Yolanda Lozano

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

After simultaneous compactification of spacetime and worldvolume on $K3$, the $D=10$ heterotic fivebrane with gauge group $SO(32)$ behaves like a $D=6$ heterotic string with gauge group $SO(28) \times SU(2)$, but with Kac--Moody levels…

High Energy Physics - Theory · Physics 2009-10-28 M. J. Duff , R. Minasian

We study type IIA string theory compactified on Calabi-Yau fourfolds and heterotic string theory compactified on Calabi-Yau threefolds times a two-torus. We derive the resulting effective theories which have two space-time dimensions and…

High Energy Physics - Theory · Physics 2010-12-03 Michael Haack , Jan Louis , Monika Marquart

We examine the extent to which the action for the membrane of M-theory (the eleven-dimensional construct which underlies and unifies all of the known string theories) simplifies in the so-called Open Membrane (OM) limit, a limit which lies…

High Energy Physics - Theory · Physics 2009-11-10 J. Antonio Garcia , Alberto Guijosa , J. David Vergara

We investigate the effective worldvolume theories of branes in a background given by (the bosonic sector of) 10-dimensional massive IIA supergravity (``massive branes'') and their M-theoretic origin. In the case of the solitonic 5-brane of…

High Energy Physics - Theory · Physics 2009-10-30 E. Bergshoeff , Y. Lozano , T. Ortin

We discuss type II and type I branes at general ADE type orbifold singularities. We show that there are new phases of type I or heterotic string theory in six dimensions, involving extra tensor multiplets, which arise when small instantons…

High Energy Physics - Theory · Physics 2009-08-18 Julie D. Blum , Kenneth Intriligator

We show that there exist two 27 and one 27 bar of E6, net one D=4, N=1 chiral matter supermultiplet as zero modes localized on the intersection of two 5-branes in the E8 x E8 heterotic string theory. The smeared intersecting 5-brane…

High Energy Physics - Theory · Physics 2014-11-20 Tetsuji Kimura , Shun'ya Mizoguchi