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Related papers: Heterotic wrapping rules

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A generalization of the Maldacena conjecture asserts that Type IIB string theory on $\S^5/\Z_3$ is equivalent to a certain supersymmetric $SU(N)^3$ gauge theory with bifundamental matter. To test this assertion, we analyze the wrapped…

High Energy Physics - Theory · Physics 2010-04-07 Sergei Gukov , Mukund Rangamani , Edward Witten

We show that string duality relates M-theory on a local Calabi-Yau fourfold singularity X4 to type IIA string theory on a Calabi-Yau threefold X3 fibered over a real line, with RR 2-form fluxes turned on. The RR flux encodes how the…

High Energy Physics - Theory · Physics 2010-05-07 Mina Aganagic

We suggest that the (2,0) six dimensional field theory compactified on $S^1\times K3$ is the Matrix model description of both M-theory on $K3$ and the Heterotic string on $T^3$. This proposal is different from existing proposals for the…

High Energy Physics - Theory · Physics 2009-10-30 Micha Berkooz , Moshe Rozali

The primary purpose of these lecture notes is to explore the moduli space of type IIA, type IIB, and heterotic string compactified on a K3 surface. The main tool which is invoked is that of string duality. K3 surfaces provide a fascinating…

High Energy Physics - Theory · Physics 2008-02-03 Paul S. Aspinwall

We discuss the equivalence between Type I, Type II and Heterotic N=2 superstring theories in four dimensions. We study the effective field theory of Type I models obtained by orientifold reductions of Type IIB compactifications on…

High Energy Physics - Theory · Physics 2009-10-30 I. Antoniadis , C. Bachas , C. Fabre , H. Partouche , T. R. Taylor

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

We classify the half-supersymmetric "domain walls", i.e. branes of codimension one, in toroidally compactified IIA/IIB string theory and show to which gauged supergravity theory each of these domain walls belong. We use as input the…

High Energy Physics - Theory · Physics 2013-05-30 Eric A. Bergshoeff , Axel Kleinschmidt , Fabio Riccioni

We present dyonic multi-membrane solutions of the N=2 D=8 supergravity theory that serves as the effective field theory of the $T^2$-compactified type II superstring theory. The `electric' charge is fractional for generic asymptotic values…

High Energy Physics - Theory · Physics 2009-10-09 J. M. Izquierdo , N. D. Lambert , G. Papadopoulos , P. K. Townsend

We extend the $P$-flux analysis carried out recently on the $T^6/[\mathbb{Z}_2 \times \mathbb{Z}_2 ]$ type-II orientifold model to include all the possible non-geometric fluxes. By deriving universal T-duality rules for all the fluxes, we…

High Energy Physics - Theory · Physics 2018-01-11 Davide M. Lombardo , Fabio Riccioni , Stefano Risoli

We study ${\cal N}=2$ compactifications of heterotic string theory on the CHL orbifold $(K3\times T^2)/\mathbb{Z}_N$ with $N= 2, 3, 5, 7$. $\mathbb{Z}_N$ acts as an involution on $K3$ together with a shift of $1/N$ along one of the circles…

High Energy Physics - Theory · Physics 2016-03-23 Shouvik Datta , Justin R. David , Dieter Lust

Twisted supergravity is supergravity in a background where the bosonic ghost field takes a non-zero value. This is the supergravity counterpart of the familiar concept of twisting supersymmetric field theories. In this paper, we give…

High Energy Physics - Theory · Physics 2016-06-02 Kevin Costello , Si Li

We consider several orbifold compactifications of M-theory and their corresponding type II duals in two space-time dimensions. In particular, we show that while the orbifold compactification of M-theory on $T^9/J_9$ is dual to the orbifold…

High Energy Physics - Theory · Physics 2010-11-19 Shibaji Roy

We initiate the study of Brane Gas Cosmology (BGC) on manifolds with non-trivial holonomy. Such compactifications are required within the context of superstring theory in order to make connections with realistic particle physics. We study…

High Energy Physics - Theory · Physics 2007-05-23 Damien A. Easson

Under the six-dimensional heterotic/type $IIA$ duality map, a solitonic membrane solution of heterotic string theory transforms into a singular solution of type $IIA$ theory, and should therefore be interpreted as a fundamental membrane in…

High Energy Physics - Theory · Physics 2014-11-18 Ramzi R. Khuri

For heterotic string theory compactified on T^6, we derive the complete set of T-duality invariants which characterize a pair of charge vectors (Q,P) labelling the electric and magnetic charges of the dyon. Using this we can identify the…

High Energy Physics - Theory · Physics 2009-09-15 Shamik Banerjee , Ashoke Sen

The string landscape satisfies interesting finiteness properties imposed by supersymmetry and string-theoretical consistency conditions. We study N=1 supersymmetric compactifications of Type IIB string theory on smooth elliptically fibered…

High Energy Physics - Theory · Physics 2015-06-19 Mirjam Cvetič , James Halverson , Denis Klevers , Peng Song

We discuss some general properties of "defect branes", i.e. branes of co-dimension two, in (toroidally compactified) IIA/IIB string theory. In particular, we give a full classification of the supersymmetric defect branes in dimensions 2 < D…

High Energy Physics - Theory · Physics 2015-05-30 E. Bergshoeff , T. Ortin , F. Riccioni

We examine the T-duality relation between 1+1 NCOS and the DLCQ limit of type IIA string theory. We show that, as long as there is a compact dimension, one can meaningfully define an `NCOS' limit of IIB/A string theory even in the absence…

High Energy Physics - Theory · Physics 2009-10-31 Ulf H. Danielsson , Alberto Guijosa , Martin Kruczenski

We construct families of supersymmetric AdS$_3\times Y_7$ and AdS$_3\times Y_8$ solutions to type IIB string theory and M-theory, respectively. Here $Y_7$ is an $S^5$ fibration over $\Sigma$, while $Y_8$ is an $S^4$ fibration over…

High Energy Physics - Theory · Physics 2021-08-20 Andrea Boido , Juan Manuel Pérez Ipiña , James Sparks

A while ago, examples of N=1 vacua in D=6 were constructed as orientifolds of Type IIB string theory compactified on the K3 surface. Among the interesting features of those models was the presence of D5-branes behaving like small…

High Energy Physics - Theory · Physics 2009-10-30 Eric G. Gimon , Clifford V. Johnson