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We study F-theory duals of six dimensional heterotic vacua in extreme regions of moduli space where the heterotic string is very strongly coupled. We demonstrate how to use orientifold limits of these F-theory duals to regain a perturbative…

High Energy Physics - Theory · Physics 2009-10-31 P. Berglund , E. G. Gimon

T-duality is a symmetry of the heterotic string to all orders in string perturbation theory. This results in an effective four dimensional supergravity theory with desirable features for phenomenology. T-duality, as well as, generically, an…

High Energy Physics - Theory · Physics 2015-05-14 Mary K. Gaillard

String theory contains sources like orientifold planes that support higher derivative interactions. These interactions make possible static flux compactifications which are forbidden in supergravity. They can also lead to violations of the…

High Energy Physics - Theory · Physics 2014-12-19 Stephen R. Green , Emil J. Martinec , Callum Quigley , Savdeep Sethi

We establish a symmetry map which relates two low-energy heterotic string theories with different numbers of the Abelian gauge fields compactified from the diverse to three dimensions on a torus. We discuss two applications of the…

High Energy Physics - Theory · Physics 2007-05-23 Oleg V. Kechkin

Special solutions of string theory in supercritical dimensions can interpolate in time between theories with different numbers of spacetime dimensions (via dimension quenching) and different amounts of worldsheet supersymmetry (via…

High Energy Physics - Theory · Physics 2008-11-26 Simeon Hellerman , Ian Swanson

The data required for heterotic string theory with gauge group G, which for anomaly cancellation reasons must either be E8 x E8 or Spin(32)/Z2, consist of the following: a ten-dimensional space-time X and a principal G-bundle P. The fields…

Differential Geometry · Mathematics 2007-05-23 Adrian Clingher

In this paper we discuss some aspects of N=1 type I-heterotic string duality in four dimensions. We consider a particular example of a (weak-weak) dual pair where on the type I side there are only D9-branes corresponding to perturbative…

High Energy Physics - Theory · Physics 2009-10-30 Zurab Kakushadze

We discuss the duality between two type I compactifications to four dimensions and an heterotic construction with spontaneous breaking of the N=4 supersymmetry to N=2. This duality allows us to gain insight into the non-perturbative…

High Energy Physics - Theory · Physics 2007-05-23 Andrea Gregori

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 discuss solutions of the heterotic string theory which are analogous to bosonic and superstring backgrounds related to coset conformal field theories. A class of exact `left-right symmetric' solutions is obtained by supplementing the…

High Energy Physics - Theory · Physics 2009-09-25 A. Giveon , E. Rabinovici , A. A. Tseytlin

The conjectured equivalence of the heterotic string to a $K_3$ compactified type IIA superstring is combined with the conjectured equivalence of the latter to a compactified 11-dimensional supermembrane to derive a string membrane duality…

High Energy Physics - Theory · Physics 2010-11-01 P. K. Townsend

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

The past year has seen enormous progress in string theory. It has become clear that all of the different string theories are different limits of a single theory. Moreover, in certain limits, one obtains a new, eleven-dimensional structure…

High Energy Physics - Theory · Physics 2007-05-23 Michael Dine

We test type IIA-heterotic string duality in six dimensions by showing that the sigma model anomaly of the heterotic string is generated by a combination of a tree level and a string one-loop correction on the type IIA side.

High Energy Physics - Theory · Physics 2010-04-07 Cumrun Vafa , Edward Witten

Classical solutions of equations of motion in low energy effective field theory, describing fundamental charged heterotic string, are found. These solutions automatically carry an electric current equal to the charge per unit length, and…

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

A strong-weak coupling duality symmetry of the string equations of motion has been suggested in the literature. This symmetry implies that vacua occur in pairs. Since the coupling constant is a dynamical variable in string theory, tunneling…

High Energy Physics - Theory · Physics 2011-06-10 J. D. Cohn , Vipul Periwal

We study the noncritical two-dimensional heterotic string. Long fundamental strings play a crucial role in the dynamics. They cancel anomalies and lead to phase transitions when the system is compactified on a Euclidean circle. A careful…

High Energy Physics - Theory · Physics 2009-11-11 Nathan Seiberg

Exact solutions of heterotic string theory corresponding to four-dimensional charge Q magnetic black holes are constructed as tensor products of an SU(2)/Z(2Q+2) WZW orbifold with a (0,1) supersymmetric SU(1,1)/U(1) WZW coset model. The…

High Energy Physics - Theory · Physics 2009-09-17 S. B. Giddings , J. Polchinski , A. Strominger

We explore the possibility of string theories in only four spacetime dimensions without any additional compactified dimensions. We show that, provided the theory is defined in curved spacetime that has a cosmological interpration, it is…

High Energy Physics - Theory · Physics 2008-11-26 Itzhak Bars

We show that in heterotic string theory compactified on a six dimensional torus, the lower bound (Bogomol'nyi bound) on the dyon mass is invariant under the SL(2,Z) transformation that interchanges strong and weak coupling limits of the…

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