Supergravity backgrounds for deformations of AdSn×Sn supercoset string models

We consider type IIB supergravity backgrounds corresponding to the deformed AdSn×Sn×T10−2n supercoset string models of the type constructed in arXiv:1309.5850 [2] which depend on one deformation parameter κ. In AdS2×S2 case we find that the deformed metric can be extended to a full supergravity solu...

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Main Authors: O. Lunin, R. Roiban, A.A. Tseytlin
Format: Article
Language:English
Published: Elsevier 2015-02-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321314003757
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spelling doaj-e8e3043db2164cb4996cb250cafd12472020-11-24T23:09:59ZengElsevierNuclear Physics B0550-32132015-02-01891106127Supergravity backgrounds for deformations of AdSn×Sn supercoset string modelsO. Lunin0R. Roiban1A.A. Tseytlin2Department of Physics, University at Albany (SUNY), Albany, NY 12222, USA; Corresponding author.Department of Physics, The Pennsylvania State University, University Park, PA 16802, USA; Kavli Institute for Theoretical Physics, University of California, Santa Barbara, CA 93106, USAThe Blackett Laboratory, Imperial College, London SW7 2AZ, UKWe consider type IIB supergravity backgrounds corresponding to the deformed AdSn×Sn×T10−2n supercoset string models of the type constructed in arXiv:1309.5850 [2] which depend on one deformation parameter κ. In AdS2×S2 case we find that the deformed metric can be extended to a full supergravity solution with non-trivial dilaton, RR scalar and RR 5-form strength. The solution depends on a free parameter a that should be chosen as a particular function of κ to correspond to the deformed supercoset model. In AdS3×S3 case the full solution supported by the dilaton, RR scalar and RR 3-form strength exists only in the two special cases, a=0 and a=1. We conjecture that there may be a more general one-parameter solution supported by several RR fields that for particular a=a(κ) corresponds to the supercoset model. In the most complicated deformed AdS5×S5 case we were able to find only the expressions for the dilaton and the RR scalar. The full solution is likely to be supported by a combination of the 5-form and 3-form field strengths. We comment on the singularity structure of the resulting metric and exact dilaton field.http://www.sciencedirect.com/science/article/pii/S0550321314003757
collection DOAJ
language English
format Article
sources DOAJ
author O. Lunin
R. Roiban
A.A. Tseytlin
spellingShingle O. Lunin
R. Roiban
A.A. Tseytlin
Supergravity backgrounds for deformations of AdSn×Sn supercoset string models
Nuclear Physics B
author_facet O. Lunin
R. Roiban
A.A. Tseytlin
author_sort O. Lunin
title Supergravity backgrounds for deformations of AdSn×Sn supercoset string models
title_short Supergravity backgrounds for deformations of AdSn×Sn supercoset string models
title_full Supergravity backgrounds for deformations of AdSn×Sn supercoset string models
title_fullStr Supergravity backgrounds for deformations of AdSn×Sn supercoset string models
title_full_unstemmed Supergravity backgrounds for deformations of AdSn×Sn supercoset string models
title_sort supergravity backgrounds for deformations of adsn×sn supercoset string models
publisher Elsevier
series Nuclear Physics B
issn 0550-3213
publishDate 2015-02-01
description We consider type IIB supergravity backgrounds corresponding to the deformed AdSn×Sn×T10−2n supercoset string models of the type constructed in arXiv:1309.5850 [2] which depend on one deformation parameter κ. In AdS2×S2 case we find that the deformed metric can be extended to a full supergravity solution with non-trivial dilaton, RR scalar and RR 5-form strength. The solution depends on a free parameter a that should be chosen as a particular function of κ to correspond to the deformed supercoset model. In AdS3×S3 case the full solution supported by the dilaton, RR scalar and RR 3-form strength exists only in the two special cases, a=0 and a=1. We conjecture that there may be a more general one-parameter solution supported by several RR fields that for particular a=a(κ) corresponds to the supercoset model. In the most complicated deformed AdS5×S5 case we were able to find only the expressions for the dilaton and the RR scalar. The full solution is likely to be supported by a combination of the 5-form and 3-form field strengths. We comment on the singularity structure of the resulting metric and exact dilaton field.
url http://www.sciencedirect.com/science/article/pii/S0550321314003757
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AT rroiban supergravitybackgroundsfordeformationsofadsnsnsupercosetstringmodels
AT aatseytlin supergravitybackgroundsfordeformationsofadsnsnsupercosetstringmodels
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