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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

The connection between IIA superstring theory compactified on a circle of radius R and IIB theory compactified on a circle of radius 1/R is reexamined from the perspective of N=2, D=9 space-time supersymmetry. We argue that the consistency…

High Energy Physics - Theory · Physics 2009-10-07 Mohab Abou-Zeid , Bernard de Wit , Dieter Lust , Hermann Nicolai

We revisit type II$_0$ limits in the vector multiplet moduli space of compactifications of Type IIB string theory on Calabi-Yau threefolds. These limits are special because they cannot be described using mirror symmetry. While we showed in…

High Energy Physics - Theory · Physics 2026-03-16 Jeroen Monnee , Timo Weigand , Max Wiesner

It is shown that the Type IIA superstring compactified on $K3$ has a smooth string soliton with the same zero mode structure as the heterotic string compactified on a four torus, thus providing new evidence for a conjectured exact duality…

High Energy Physics - Theory · Physics 2009-09-17 J. A. Harvey , A. Strominger

The nature of M-theory on K3 X I, where I is a line interval, is considered, with a view towards formulating a `matrix theory' representation of that situation. Various limits of this compactification of M-theory yield a number of well…

High Energy Physics - Theory · Physics 2009-10-30 Clifford V. Johnson

We define an algebra on the space of BPS states in theories with extended supersymmetry. We show that the algebra of perturbative BPS states in toroidal compactification of the heterotic string is closely related to a generalized Kac-Moody…

High Energy Physics - Theory · Physics 2010-11-19 Jeffrey A. Harvey , Gregory Moore

We demonstrate that type II string theory compactified on a singular Calabi-Yau manifold is related to $c=1$ string theory compactified at the self-dual radius. We establish this result in two ways. First we show that complex structure…

High Energy Physics - Theory · Physics 2009-10-28 Dileep P. Jatkar , Bas Peeters

It is shown how the topological string amplitudes encode the BPS structure of wrapped M2 branes in M-theory compactification on Calabi-Yau threefolds. This in turn is related to a twisted supersymmetric index in 5 dimensions which receives…

High Energy Physics - Theory · Physics 2007-05-23 Rajesh Gopakumar , Cumrun Vafa

We study the compactification of the $(2,0)$ and type-II little-string theories on $S^1$, $T^2$ and $T^3$ with an R-symmetry twist that preserves half the supersymmetry. We argue that it produces the same moduli spaces of vacua as…

High Energy Physics - Theory · Physics 2009-10-31 Yeuk-Kwan E. Cheung , Ori J. Ganor , Morten Krogh

We explicitly give the correspondence between spectra of heterotic string theory compactified on $T^2$ and string junctions in type IIB theory compactified on $S^2$.

High Energy Physics - Theory · Physics 2008-11-26 Yosuke Imamura

Considering SO(32) heterotic string theory compactified on a torus of dimension 4 and less, stability of non-supersymmetric states is studied. A non-supersymmetric state with robust stability is constructed, and its exact stability is…

High Energy Physics - Theory · Physics 2015-06-05 Jihye Seo

We derive a formula for D3-brane charge on a compact spacetime, which includes torsion corrections to the tadpole cancellation condition. We use this to classify D-branes and RR fluxes in type II string theory on RP^3xRP^{2k+1}xS^{6-2k}…

High Energy Physics - Theory · Physics 2007-05-23 P. Bouwknegt , J. Evslin , B. Jurco , V. Mathai , H. Sati

We show that the supermembrane theory compactified on a torus is invariant under T-duality. There are two different topological sectors of the compactified supermembrane (M2) classified according to a vanishing or nonvanishing second…

High Energy Physics - Theory · Physics 2016-11-23 M. P. Garcia del Moral , J. M. Pena , A. Restuccia

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

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 consider the compactification of the E8xE8 heterotic string on a K3 surface with "the spin connection embedded in the gauge group" and the dual picture in the type IIA string (or F-theory) on a Calabi-Yau threefold X. It turns out that…

High Energy Physics - Theory · Physics 2008-11-26 Paul S. Aspinwall , Ron Y. Donagi

In this note I review the role played by dualities in the Supermembrane Theory compactified on a torus. Supermembrane theory realize S, T, so U-duality, as exact symmetries of the theory. There are two well defined sectors: with and without…

High Energy Physics - Theory · Physics 2012-11-28 M. P. Garcia del Moral

We study quantum effects in five dimensions in heterotic superstring theory compactified on K_3 x S_1 and analyze the conjecture that its dual effective theory is eleven-dimensional supergravity compactified on a Calabi-Yau threefold. This…

High Energy Physics - Theory · Physics 2011-05-05 I. Antoniadis , S. Ferrara , T. R. Taylor

After a short introduction to Matrix theory, we explain how can one generalize matrix models to describe toroidal compactifications of M-theory and the heterotic vacua with 16 supercharges. This allows us, for the first time in history, to…

High Energy Physics - Theory · Physics 2007-05-23 Lubos Motl

Ten dimensional type IIA and IIB theories with p-branes are compactified to 8-dimensions. It is shown that resulting branes can be classified according to the representations of $\bf {SL(3,Z) \times SL(2,Z)}$. These p-branes can also be…

High Energy Physics - Theory · Physics 2014-11-18 Jnanadeva Maharana