Refined topological amplitudes from the Ω-background in string theory

被引:2
|
作者
Angelantonj, Carlo [1 ,2 ,3 ]
Antoniadis, Ignatios [4 ,5 ,6 ]
Florakis, Ioannis [7 ,8 ]
Jiang, Hongliang [9 ]
机构
[1] Univ Torino, Dipartimento Fis, Via Pietro Giuria 1, I-10125 Turin, Italy
[2] INFN Sez Torino, Via Pietro Giuria 1, I-10125 Turin, Italy
[3] Arnold Regge Ctr, Via Pietro Giuria 1, I-10125 Turin, Italy
[4] Sorbonne Univ, CNRS, LPTHE, Lab Phys Theor & Hautes Energies, 4 Pl Jussieu, F-75005 Paris, France
[5] Stockholm Univ, Nordita, Hannes Alfvens Vag 12, S-10691 Stockholm, Sweden
[6] KTH Royal Inst Technol, Hannes Alfvens Vag 12, S-10691 Stockholm, Sweden
[7] Univ Liverpool, Dept Math Sci, Liverpool L69 7ZL, Merseyside, England
[8] Univ Ioannina, Dept Phys, Ioannina 45110, Greece
[9] Queen Mary Univ London, Dept Phys & Astron, Ctr Theoret Phys, Mile End Rd, London E1 4NS, England
基金
英国科学技术设施理事会;
关键词
Superstrings and Heterotic Strings; Topological Strings; PARTITION-FUNCTION; SUPERSYMMETRY; REALIZATION; BREAKING;
D O I
10.1007/JHEP05(2022)143
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
It was recently shown that the N = 2 string topological amplitudes in the heterotic weak coupling limit generate a six-dimensional Melvin space, providing a description of the Omega-background in string theory, where string propagation can be exactly studied. In this work, we generalise the analysis to the refined case of the Omega-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.
引用
收藏
页数:18
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