Refined topological amplitudes from the Ω-background in string theory

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作者
Carlo Angelantonj
Ignatios Antoniadis
Ioannis Florakis
Hongliang Jiang
机构
[1] Dipartimento di Fisica,Department of Mathematical Sciences
[2] Università di Torino,Department of Physics
[3] and INFN Sezione di Torino,Centre for Theoretical Physics, Department of Physics and Astronomy
[4] Arnold-Regge Center,undefined
[5] Laboratoire de Physique Théorique et Hautes Énergies — LPTHE,undefined
[6] Sorbonne Université,undefined
[7] CNRS,undefined
[8] Nordita,undefined
[9] Stockholm University and KTH Royal Institute of Technology,undefined
[10] University of Liverpool,undefined
[11] University of Ioannina,undefined
[12] Queen Mary University of London,undefined
关键词
Superstrings and Heterotic Strings; Topological Strings;
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摘要
It was recently shown that the N\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathcal{N} $$\end{document} = 2 string topological amplitudes in the heterotic weak coupling limit generate a six-dimensional Melvin space, providing a description of the Ω-background in string theory, where string propagation can be exactly studied. In this work, we generalise the analysis to the refined case of the Ω-background with two independent deformation parameters. The Melvin space is now ten-dimensional and is extended by an action on the internal K3 compactification manifold of the heterotic superstring, corresponding to an SU(2)R rotation in the field theory description. We identify the class of heterotic topological amplitudes realising this background as the scattering of two anti-self-dual gravitons and arbitrary numbers of anti-self-dual graviphotons, self-dual vector fields of the dilaton multiplet, together with self-dual magnetic fluxes along the K3. In the field theory limit, our result correctly reproduces the perturbative part of the Nekrasov free energy in the case where both equivariant parameters are turned on.
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