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We discuss the physical superstring correlation functions in type I theory (or equivalently type II with orientifold) that compute real topological string amplitudes. We consider the correlator corresponding to holomorphic derivative of the…

High Energy Physics - Theory · Physics 2017-03-17 K. S. Narain , N. Piazzalunga , A. Tanzini

We generalize to the case of compactified superstrings a construction given previously for critical superstrings of finite one loop amplitudes that are well-defined for all external momenta. The novel issues that arise for compactified…

High Energy Physics - Theory · Physics 2009-10-30 Gordon Chalmers

We show that certain heterotic string amplitudes are given in terms of correlators of the twisted topological (2,0) SCFT, corresponding to the internal sector of the N=1 spacetime supersymmetric background. The genus g topological partition…

High Energy Physics - Theory · Physics 2009-10-30 I. Antoniadis , E. Gava , K. S. Narain , T. R. Taylor

In any string theory there is a hidden, twisted superconformal symmetry algebra, part of which is made up by the BRST current and the anti-ghost. We investigate how this algebra can be systematically constructed for strings with $N\!-\!2$…

High Energy Physics - Theory · Physics 2009-10-28 A. Boresch , K. Landsteiner , W. Lerche , A. Sevrin

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 describe a topological string theory which reproduces many aspects of the 1/N expansion of SU(N) Yang-Mills theory in two spacetime dimensions in the zero coupling (A=0) limit. The string theory is a modified version of topological…

High Energy Physics - Theory · Physics 2009-10-28 Stefan Cordes , Gregory Moore , Sanjaye Ramgoolam

We consider compactifications of the heterotic string on $K3 \times T2$ so that the resulting theory in $d = 4$ space-time dimensions has $N = 2$ supersymmetry. The gravitational and gauge coupling constants of the low-energy effective…

High Energy Physics - Theory · Physics 2009-10-30 M. Henningson , G. Moore

We investigate the connections between four-dimensional, N=2 M-theory vacua constructed as orbifolds of type II, heterotic, and type I strings. All these models have the same massless spectrum, which contains an equal number of vector…

High Energy Physics - Theory · Physics 2009-10-31 Andrea Gregori , Costas Kounnas

We show a possibility that the matrix models recently proposed to explain (almost) all the physics of M-theory may include the superstring theories that we know perturbatively. The ``1st quantized'' physical system of one IIA string seems…

High Energy Physics - Theory · Physics 2008-02-03 Lubos Motl

We analyze topological string theory on a two dimensional torus, focusing on symmetries in the matter sector. Even before coupling to gravity, the topological torus has an infinite number of point-like physical observables, which give rise…

High Energy Physics - Theory · Physics 2009-10-22 Petr Horava

A worldsheet realization of the refined topological string is proposed in terms of physical string amplitudes that compute generalized N=2 F-terms of the form F_{g,n} W^{2g}Y^{2n} in the effective supergravity action. These terms involve…

High Energy Physics - Theory · Physics 2013-08-01 I. Antoniadis , I. Florakis , S. Hohenegger , K. S. Narain , A. Zein Assi

We derive the three-dimensional $\mathcal{N}=1$ effective theories obtained by compactifying all five ten-dimensional string theories on generic seven-dimensional manifolds with $G_2$ structure. The resulting flux compactifications are…

High Energy Physics - Theory · Physics 2026-05-11 Aravind Aikot , Zheng Miao , George Tringas , Timm Wrase

We prove that critical and subcritical N=2 string theory gives a realization of an N=2 superfield extension of the topological conformal algebra. The essential observation is the vanishing of the background charge.

High Energy Physics - Theory · Physics 2009-10-22 J. Gomis , H. Suzuki

The target space theory of the N=(2,1) heterotic string may be interpreted as a theory of gravity coupled to matter in either $1+1$ or $2+1$ dimensions. Among the target space theories in $1+1$ dimensions are the bosonic, type II, and…

High Energy Physics - Theory · Physics 2009-10-30 D. Kutasov , E. Martinec

We show the existence of a global anomaly in the one-loop graphs of N=2 string theory, defined by sewing tree amplitudes, unless spacetime supersymmetry is imposed. The anomaly is responsible for the non-vanishing maximally helicity…

High Energy Physics - Theory · Physics 2009-10-31 Gordon Chalmers , Warren Siegel

Perturbative string amplitudes are correctly derived from the string geometry theory, which is one of the candidates of a non-perturbative formulation of string theory. In order to derive non-perturbative effects rather easily, we formulate…

High Energy Physics - Theory · Physics 2020-10-15 Matsuo Sato , Yuji Sugimoto

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

We outline a general geometric structure that underlies the N=1 superpotentials of a certain class of flux and brane configurations in type II string compactifications on Calabi-Yau threefolds. This ``holomorphic N=1 special geometry'' is…

High Energy Physics - Theory · Physics 2007-05-23 W. Lerche , P. Mayr , N. Warner

We review some examples of heterotic/type II string duality which shed light on the infrared dynamics of string compactifications with N=2 and N=1 supersymmetry in four dimensions.

High Energy Physics - Theory · Physics 2007-05-23 Shamit Kachru

It is shown that the generating function of $\mathscr{N}=2$ topological strings, in the heterotic weak coupling limit, is identified with the partition function of a six-dimensional Melvin background. This background, which corresponds to…

High Energy Physics - Theory · Physics 2020-01-29 Carlo Angelantonj , Ignatios Antoniadis