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Related papers: Non-perturbative triality in heterotic and type II…

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We discuss type I -- heterotic duality in four-dimensional models obtained as a Coulomb phase of the six-dimensional U(16) orientifold model compactified on T^2 with arbitrary SU(16) Wilson lines. We show that Kahler potentials, gauge…

High Energy Physics - Theory · Physics 2014-11-18 I. Antoniadis , H. Partouche , T. R. Taylor

We analyze the U-duality group for the case of a type II superstring compactified to four dimensions on a K3 surface times a torus. The various limits of this theory are considered which have interpretations as type IIA and IIB…

High Energy Physics - Theory · Physics 2010-11-01 Paul S. Aspinwall , David R. Morrison

We give necessary conditions for the existence of perturbative heterotic and common sector type II string warped compactifications preserving four and eight supersymmetries to four spacetime dimensions, respectively. In particular, we find…

High Energy Physics - Theory · Physics 2009-10-09 S. Ivanov , G. Papadopoulos

The condition of having an $N=1$ spacetime supersymmetry for heterotic string leads to 4 distinct possibilities for compactifications namely compactifications down to 6,4,3 and 2 dimensions. Compactifications to 6 and 4 dimensions have been…

High Energy Physics - Theory · Physics 2010-11-01 S. L. Shatashvili , C. Vafa

We re-examine the question of heterotic - heterotic string duality in six dimensions and argue that the $E_8\times E_8$ heterotic string, compactified on $K3$ with equal instanton numbers in the two $E_8$'s, has a self-duality that inverts…

High Energy Physics - Theory · Physics 2010-04-07 M. J. Duff , R. Minasian , Edward Witten

The perturbative prepotential and the K\"ahler metric of the vector multiplets of the N=2 effective low-energy heterotic strings is calculated directly in N=1 six-dimensional toroidal compactifications of the heterotic string vacua. This…

High Energy Physics - Theory · Physics 2014-11-18 Christos kokorelis

Motivated by the study of black attractors in 8D supergravity with 16 supersymmetries, we use the field theory approach and 8D supersymmetry with non trivial central charges to shed light on the exact duality between heterotic string on T^2…

High Energy Physics - Theory · Physics 2015-03-17 El Hassan Saidi

The perturbative prepotential and the K\"ahler metric of the vector multiplets of the N=2 effective low-energy heterotic strings is calculated directly in N=1 six-dimensional toroidal compactifications of the heterotic string vacua. This…

High Energy Physics - Theory · Physics 2007-05-23 Christos Kokorelis

In this paper we summarize our recent work about perturbative and non-perturbative effects in four-dimensional heterotic strings with $N=2$ space-time supersymmetry.

High Energy Physics - Theory · Physics 2009-10-28 G. Lopes Cardoso , D. Lust , T. Mohaupt

Recent work on four dimensional effective descriptions of the heterotic string has identified the moduli of such systems as being given by kernels of maps between ordinary Dolbeault cohomology groups. The maps involved are defined by the…

High Energy Physics - Theory · Physics 2018-08-15 James Gray , Hadi Parsian

We propose non-supersymmetric analogues of 6d N=2 Type II/heterotic dualities via a quotient of a K3 surface: an Enriques surface. We start from Type~II strings on a K3 surface and construct orbifold theories using an involution of K3. We…

High Energy Physics - Theory · Physics 2026-01-30 Arata Ishige

We study orbifolds by permutations of two identical N=2 minimal models within the Gepner construction of four dimensional heterotic strings. This is done using the new N=2 supersymmetric permutation orbifold building blocks we have recently…

High Energy Physics - Theory · Physics 2011-08-03 M. Maio , A. N. Schellekens

We discuss the mathematical properties of six--dimensional non--K\"ahler manifolds which occur in the context of ${\cal N}=1$ supersymmetric heterotic and type IIA string compactifications with non--vanishing background H--field. The…

High Energy Physics - Theory · Physics 2009-10-07 G. L. Cardoso , G. Curio , G. Dall'Agata , D. Lust , P. Manousselis , G. Zoupanos

The heterotic string theory, compactified to four dimensions, has been conjectured to have a duality symmetry (S duality) that transforms the dilaton nonlinearly. If valid, this symmetry could provide an important means of obtaining…

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

Using free world-sheet fermions, we construct and classify all the N=2, Z2 X Z2 four-dimensional orbifolds of the type IIA/B strings for which the orbifold projections act symmetrically on the left and right movers. We study the…

High Energy Physics - Theory · Physics 2009-10-31 A. Gregori , C. Kounnas , J. Rizos

In this thesis, we explore two approaches to string phenomenology. In the first half of the work, we investigate M-theory compactifications on spaces with co-dimension four, orbifold singularities. We construct M-theory on C^2/Z_N by…

High Energy Physics - Theory · Physics 2008-08-28 Lara B. Anderson

We analyze the map between heterotic and type II N=2 supersymmetric string theories for certain two and three moduli examples found by Kachru and Vafa. The appearance of elliptic j-functions can be traced back to specializations of the…

High Energy Physics - Theory · Physics 2009-10-28 A. Klemm , W. Lerche , P. Mayr

We study supersymmetric compactification to four dimensions with non-zero H-flux in heterotic string theory. The background metric is generically conformally balanced and can be conformally Kahler if the primitive part of the H-flux…

High Energy Physics - Theory · Physics 2008-11-26 Katrin Becker , Li-Sheng Tseng

We study a class of extremal transitions between topological distinct Calabi--Yau manifolds which have an interpretation in terms of the special massless states of a type II string compactification. In those cases where a dual heterotic…

High Energy Physics - Theory · Physics 2009-10-30 A. Klemm , P. Mayr

We review the construction of open descendants of the type IIB superstring on the Z-orbifold. It results in a chiral four-dimensional model with gauge group $SO(8) \otimes U(12)$ and three generations of matter in the $(8,12^*)\oplus…

High Energy Physics - Theory · Physics 2010-11-19 Carlo Angelantonj