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Related papers: M(atrix) String Theory on K3

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Type II compactifications with varying string coupling can be described elegantly in F-theory/M-theory as compactifications on U - manifolds. Using a similar approach to describe Super Yang-Mills with a varying coupling constant, we argue…

High Energy Physics - Theory · Physics 2009-10-30 Suresh Govindarajan

In this note we compare the moduli spaces of the heterotic string compactified on a two-torus and F-Theory compactified on an elliptic K3 surface for the case of an unbroken E8 x E8 gauge group. The explicit map relating the deformation…

High Energy Physics - Theory · Physics 2009-10-07 Gabriel Lopes Cardoso , Gottfried Curio , Dieter Lust , Thomas Mohaupt

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 study the Matrix theory description of M-theory compactified on $T^4$ and $T^5$. M-theory on $T^4$ is described by the six dimensional (2,0) fixed point field theory compactified on a five torus, $\widetilde T^5$. For M-theory on $T^5$…

High Energy Physics - Theory · Physics 2009-09-15 Micha Berkooz , Moshe Rozali , Nathan Seiberg

We study the duality between M-theory compactified on Calabi-Yau fourfolds and the heterotic string compactified on Calabi-Yau threefolds times a circle. Our analysis is based on a comparison of the low energy effective actions in three…

High Energy Physics - Theory · Physics 2007-05-23 Michael Haack , Jan Louis

Using a recently constructed M5-brane world-volume action, we demonstrate that wrapping the M5-brane on K3 gives the heterotic string in seven dimensions. To facilitate the comparison, a new version of the world-sheet action for the…

High Energy Physics - Theory · Physics 2009-02-11 Sergey Cherkis , John H. Schwarz

The principle of equivalence is translated into the language of the world-volume field theories that define matrix and string theories. This idea leads to explore possible matrix descriptions of M-theory compactifications. An interesting…

High Energy Physics - Theory · Physics 2007-05-23 Jesús Puente Peñalba

We analyze the structure of heterotic M-theory on K3 orbifolds by presenting a comprehensive sequence of M-theoretic models constructed on the basis of local anomaly cancellation. This is facilitated by extending the technology developed in…

High Energy Physics - Theory · Physics 2009-10-07 M. Faux , D. Lust , B. A. Ovrut

We review some recent developments in the study of M-theory compactifications via Matrix theory. In particular we highlight the appearance of IIA strings and their interactions, and explain the unifying role of the M-theory five-brane for…

High Energy Physics - Theory · Physics 2009-10-30 R. Dijkgraaf , E. Verlinde , H. Verlinde

We discuss N=2 supersymmetric compactifications to four dimensions from the point of view of F-theory and heterotic theory. In a relatively simple setup, we illustrate the spectral theory for vector bundles on K3xT^2 and discuss the…

High Energy Physics - Theory · Physics 2009-10-30 Michael Bershadsky , Vladimir Sadov

This is a summary of a talk at Strings2000 explaining three ways in which string theory and M-theory are related to the mathematics of K-theory.

High Energy Physics - Theory · Physics 2015-06-25 Gregory Moore

M-theory on K3xK3 with non-supersymmetry-breaking G-flux is dual to M-theory on a Calabi-Yau threefold times a 2-torus without flux. This allows for a thorough analysis of the effects of flux without relying on supergravity approximations.…

High Energy Physics - Theory · Physics 2007-05-23 Paul S. Aspinwall

I discuss the relation between M-theory and M(atrix)-theory in flat space by considering the effective potential for the scattering of two groups of D0-branes in both theories. An explicit calculation of this potential up to two loop order…

High Energy Physics - Theory · Physics 2009-10-30 Katrin Becker

I review the appearance, within Matrix theory, of the $SL(5,Z)$ U-duality group of M-theory on $T^4$, and the duality between M-theory on K3 and the Heterotic string on $T^3$. In both cases the duality is geometrical and manifest.

High Energy Physics - Theory · Physics 2009-10-30 Micha Berkooz

It is shown that many of the conjectured dualities involving orbifold compactification of M-theory follow from the known dualities involving M-theory and string theory in ten dimensions, and the ansatz that orbifolding procedure commutes…

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

We study the M(atrix) theory which describes the $E_8 \times E_8$ heterotic string compactified on $S^1$, or equivalently M-theory compactified on an orbifold $(S^1/\integer_2) \times S^1$, in the presence of a Wilson line. We formulate the…

High Energy Physics - Theory · Physics 2008-11-26 Daniel Kabat , Soo-Jong Rey

We study string theory propagating on R^6 times K3 by constructing orientifolds of Type IIB string theory compactified on the T^4/Z_N orbifold limits of the K3 surface. This generalises the Z_2 case studied previously. The orientifold…

High Energy Physics - Theory · Physics 2014-11-18 Eric G. Gimon , Clifford V. Johnson

We study compactifications of string theory and M-theory to six dimensions with background fluxes. The nonzero fluxes lead to additional mass parameters. We derive the S- and T-duality rules for the corresponding (massive) supergravity…

High Energy Physics - Theory · Physics 2008-12-18 K. Behrndt , E. Bergshoeff , D. Roest , P. Sundell

We compare the $(0,2)$ theory of the single M5 brane decoupled from gravity in the lightcone with transverse $R^4$, and a matrix model description in terms of quantum mechanics on instanton moduli space. We give some tests of the Matrix…

High Energy Physics - Theory · Physics 2009-10-30 J. Brodie , S. Ramgoolam

We study the strong coupling dynamics of the heterotic E_8 x E_8 string theory on the orbifolds T^6/Z_3 and C^3/Z_3 using the duality with the Horava-Witten M-theory picture. This leads us to a conjecture about the low energy description of…

High Energy Physics - Theory · Physics 2014-11-18 O. J. Ganor , J. Sonnenschein