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Related papers: String duality and massless string states

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We investigate the perturbative and non-perturbative correspondence of a class of four dimensional dual string constructions with N=4 and N=2 supersymmetry, obtained as Z_2 or Z_2 x Z_2 orbifolds of the type II, heterotic and type I string.…

High Energy Physics - Theory · Physics 2010-02-03 Andrea Gregori

We discuss the predictions of S-duality for the monopole spectrum of four-dimensional heterotic string theory resulting from toroidal compactification. We discuss in detail the spectrum of "H-monopoles", states that are magnetically charged…

High Energy Physics - Theory · Physics 2007-05-23 J. P. Gauntlett , J. A. Harvey

We examine non-abelian duality transformations in the open string case. After gauging the isometries of the target space and developing the general formalism, we study in details the duals oftarget spaces with SO(N) isometries which, for…

High Energy Physics - Theory · Physics 2014-11-18 S. Forste , A. Kehagias , S. Schwager

Massless BPS-saturated states in toroidally compactified heterotic string were discussed first. Then, I constructed a large class of BPS-saturated states of toroidally compactified type II string theories. They were parametrized by four…

High Energy Physics - Theory · Physics 2007-05-23 Kwan-Leung Chan

In this lecture we review some of the recent developments in string theory on an introductory and qualitative level. In particular we focus on S-T-U dualities of toroidally compactified ten-dimensional string theories and outline the…

High Energy Physics - Theory · Physics 2014-11-18 Stefan Forste , Jan Louis

We classify almost all classical string configurations, considered in the framework of the semi-classical limit of the string/gauge theory duality. Then, we describe a procedure for obtaining the conserved quantities and the exact classical…

High Energy Physics - Theory · Physics 2007-05-23 D. Aleksandrova , P. Bozhilov

The paper discusses the connection between S-duality and string-theoretic picture-changing formalism. The singular limit of the picture-changing transformation at zero momentum leads to the presence of the topological 5-form charge in the…

High Energy Physics - Theory · Physics 2008-02-03 Dimitri Polyakov

A free superstring with chiral N=2 supersymmetry in six dimensions is proposed. It couples to a two-form gauge field with a self-dual field strength. Compactification to four dimensions on a two-torus gives a strongly coupled N=4…

High Energy Physics - Theory · Physics 2007-05-23 John H. Schwarz

We consider non-critical heterotic strings compactified on $S^1$. For full rank theories, they are related to odd self-dual lattices and are structurally of the same form as the critical non-supersymmetric theories. For dimensions up to 14…

High Energy Physics - Theory · Physics 2024-12-31 Héctor Parra De Freitas

We consider an eleven dimensional supergravity compactified on $K3\times T^2$ and show that the resulting five dimensional theory has identical massless states as that of heterotic string compactified on a specific five torus $T^5$. The…

High Energy Physics - Theory · Physics 2009-10-28 Supriya Kar , Jnanadeva Maharana , Sudhakar Panda

We review the status of duality symmetries in superstring theories. These discrete symmetries mark the striking differences between theories of pointlike objects and theories of extended objects. They prove to be very helpful in…

High Energy Physics - Theory · Physics 2011-04-15 Massimo Bianchi

We consider the effects of abelian duality transformations on static, spherically-symmetric, asymptotically flat string spacetimes in four dimensions, where the dilaton, axion, metric, and gauge fields are allowed to be nonzero. Independent…

High Energy Physics - Theory · Physics 2008-11-26 C. P. Burgess , R. C. Myers , F. Quevedo

A class of mathematical dualities have played a central role in mapping states in gauge theory to states in the spacetime string theory dual. This includes the classical Schur-Weyl duality between symmetric groups and Unitary groups, as…

High Energy Physics - Theory · Physics 2008-11-26 Sanjaye Ramgoolam

We analyze the zero mass black holes that arise as classical solutions to low energy heterotic string theory. Though these solutions contain naked singularities, it has been conjectured that they should be allowed in the theory. We find a…

High Energy Physics - Theory · Physics 2009-10-30 R. Emparan

We define generalized dualities for heterotic and type I strings based on consistent truncations to half-maximal gauged supergravities in more than three dimensions. The latter are constructed from a generalized Scherk-Schwarz ansatz in…

High Energy Physics - Theory · Physics 2024-09-24 Falk Hassler , Yuho Sakatani , Luca Scala

We extend strong/weak coupling duality to string theories without spacetime supersymmetry, and focus on the case of the unique ten-dimensional, nonsupersymmetric, tachyon-free $SO(16)\times SO(16)$ heterotic string. We construct a…

High Energy Physics - Theory · Physics 2009-08-18 Julie D. Blum , Keith R. Dienes

When the gauge groups of the two heterotic string theories are broken, over tori, to their "SO(16)x SO(16)" subgroups, the winding modes correspond to representations which are spinorial with respect to those subgroups. Globally, the two…

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

The configuration of typical highly excited (M >> M_s ~ (alpha')^{-1/2}) string states is considered as the string coupling g is adiabatically increased. The size distribution of very massive single string states is studied and the mass…

High Energy Physics - Theory · Physics 2009-10-31 Thibault Damour , Gabriele Veneziano

Using heterotic/type II string duality, we obtain exact nonperturbative results for the point particle limit (alpha' -> 0) of some particular four dimensional, N=2 supersymmetric compactifications of heterotic strings. This allows us to…

High Energy Physics - Theory · Physics 2009-10-07 S. Kachru , A. Klemm , W. Lerche , P. Mayr , C. Vafa

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