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Related papers: A note on heterotic/type I' duality and D0 brane q…

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Compactifications of the heterotic string on T^d are the simplest, yet rich enough playgrounds to uncover swampland ideas: the U(1)^{d+16} left-moving gauge symmetry gets enhanced at special points in moduli space only to certain groups. We…

High Energy Physics - Theory · Physics 2020-12-02 Anamaría Font , Bernardo Fraiman , Mariana Graña , Carmen A. Núñez , Héctor Parra De Freitas

In the string/gauge duality it is important to understand how the space-time geometry is encoded in gauge theory observables. We address this issue in the case of the D0-brane system at finite temperature T. Based on the duality, the…

High Energy Physics - Theory · Physics 2009-06-25 Masanori Hanada , Akitsugu Miwa , Jun Nishimura , Shingo Takeuchi

We develop a matrix model for the SO(32) Heterotic string with certain Wilson lines on the lightlike circle. This is done by using appropriate T-dualities. The method works for an infinite number of Wilson lines, but not for all. The matrix…

High Energy Physics - Theory · Physics 2009-10-31 Morten Krogh

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

We explore the moduli space of heterotic strings in two dimensions. In doing so, we introduce new lines of compactified theories with Spin(24) gauge symmetry and discuss compactifications with Wilson lines. The phase structure of d=2…

High Energy Physics - Theory · Physics 2008-11-26 Joshua L. Davis

We derive the moduli dependent threshold corrections to gauge couplings in toroidal orbifold compactifications. The underlying six dimensional torus lattice of the heterotic string theory is not assumed ---as in previous calculations--- to…

High Energy Physics - Theory · Physics 2010-11-01 P. Mayr , S. Stieberger

We use heterotic/type-II prepotentials to study quantum/classical black holes with half the $N=2, D=4$ supersymmetries unbroken. We show that, in the case of heterotic string compactifications, the perturbatively corrected entropy formula…

High Energy Physics - Theory · Physics 2008-11-26 K. Behrndt , G. Lopes Cardoso , B. de Wit , R. Kallosh , D. Lüst , T. Mohaupt

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

Intersecting D-brane models and their T-dual magnetic compactifications yield attractive models of particle physics where magnetic flux plays a twofold role, being the source of fermion chirality as well as supersymmetry breaking. A…

High Energy Physics - Theory · Physics 2020-02-11 Wilfried Buchmuller , Emilian Dudas , Yoshiyuki Tatsuta

We study moduli dependent threshold corrections to gravitational couplings in the case of the heterotic string compactified on a symmetric orbifold, for untwisted moduli, extending previous analysis on gauge couplings. Like in the gauge…

High Energy Physics - Theory · Physics 2010-11-01 I. Antoniadis , E. Gava , K. S. Narain

We estimate the effect of threshold corrections coming from Wilson lines to gauge coupling unification in the weakly coupled heterotic string with orbifold compactification. By expressing the corrections in terms of an effective field…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. G. Ross

We study compactification of heterotic strings to three dimensions on orbifolds of G_2 holonomy. We consider the standard embedding and show that the gauge group is broken from E_8 x E_8 or SO(32) to F_4 x E_8 or SO(25) respectively. We…

High Energy Physics - Theory · Physics 2010-12-02 Anamaria Font

Two classes of stringy instanton effects, stronger than standard field theory instantons, are identified in the heterotic string theory. These contributions are established using type IIA/heterotic and type I/heterotic dualities. They…

High Energy Physics - Theory · Physics 2009-10-30 Eva Silverstein

Heterotic string theory compactified on a K3 surface times T^2 is believed to be equivalent to type II string theory on a suitable Calabi-Yau threefold. In particular, it must share the same hypermultiplet moduli space. Building on the…

High Energy Physics - Theory · Physics 2014-09-04 Sergei Alexandrov , Boris Pioline

We perform a complete analysis of one-loop threshold corrections to the gauge couplings of fractional D6-branes. This includes besides SU(N) also symplectic, orthogonal and massless Abelian gauge factors and the full computation of…

High Energy Physics - Theory · Physics 2010-01-18 Florian Gmeiner , Gabriele Honecker

We elaborate that general intersecting brane models on orbifolds are obtained from type I string compactifications and their T-duals. Symmetry breaking and restoration occur via recombination and parallel separation of branes, preserving…

High Energy Physics - Theory · Physics 2008-11-26 Kang-Sin Choi

The effective action for type II string theory compactified on a six torus is $N=8$ supergravity, which is known to have an $E_{7}$ duality symmetry. We show that this is broken by quantum effects to a discrete subgroup, $E_7(\Z)$, which…

High Energy Physics - Theory · Physics 2009-07-09 C. M. Hull , P. K. Townsend

T-duality has been shown to constrain the higher derivative corrections of string theory. We revisit the problem of understanding the T-duality constraints imposed on the $\alpha'$ corrections using the language of a torsionful connection.…

High Energy Physics - Theory · Physics 2023-03-01 Marina David , James T. Liu

We argue that all conjectured dualities involving various string, M- and F- theory compactifications can be `derived' from the conjectured duality between type I and SO(32) heterotic string theory, T-dualities, and the definition of M- and…

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

In discussions of the T-duality between the two heterotic string theories, the duality is actually implemented through the "common" SO(16) x SO(16) subgroup of "SO(32)" and E_8 x E_8. In fact, however, a global investigation shows that no…

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