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Supergravity background of λ-deformed model for AdS 2 × S 2 supercoset

机译:λ的超重力背景- AdS 2 × S 2 超Coset

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Starting with the F ? / G supercoset model corresponding to the AdS n × S n superstring one can define the λ -model of arXiv:1409.1538 either as a deformation of the F ? / F ? gauged WZW model or as an integrable one-parameter generalisation of the non-abelian T-dual of the AdS n × S n superstring sigma model with respect to the whole supergroup F ? . Here we consider the case of n = 2 and find the explicit form of the 4d target space background for the λ -model for the PSU ( 1 , 1 | 2 ) / SO ( 1 , 1 ) × SO ( 2 ) supercoset. We show that this background represents a solution of type IIB 10d supergravity compactified on a 6-torus with only metric, dilaton Φ and the RR 5-form (represented by a 2-form F in 4d) being non-trivial. This implies that the λ -model is Weyl invariant at the quantum level and thus defines a consistent superstring sigma model. The supergravity solution we find is different from the one in arXiv:1410.1886 which should correspond to a version of the λ -model where only the bosonic subgroup of F ? is gauged. Still, the two solutions have equivalent scaling limit of arXiv:1504.07213 leading to the isometric background for the metric and e Φ F which is related to the η -deformed AdS 2 × S 2 sigma model of arXiv:1309.5850. Similar results are expected in the AdS 3 × S 3 and AdS 5 × S 5 cases.
机译:以F开头?对应于AdS n×S n超串的/ G超陪集模型可以将arXiv:1409.1538的λ模型定义为F?的变形。 / F ?规范的WZW模型或作为AdS n×S n超字符串sigma模型相对于整个超群F?的非阿贝尔T-对偶的可积一参数泛化。 。在这里,我们考虑n = 2的情况,并为PSU(1,1 | 2)/ SO(1,1)×SO(2)超集合的λ模型找到4d目标空间背景的显式形式。我们显示该背景表示在II型10d超重力压实的解决方案,其中仅以公制,dilatonΦ和RR 5形式(在4d中以2形式的F表示)被压缩在6个托勒斯上。这意味着λ-模型在量子水平上是Weyl不变的,因此定义了一个一致的超弦sigma模型。我们发现的超重力解与arXiv:1410.1886中的解不同,后者应对应于λ模型的一种形式,其中仅F?的玻色子群为?被测量。仍然,这两个解决方案具有arXiv:1504.07213的等效缩放限制,导致度量的等距背景和eΦF,这与arXiv:1309.5850的η变形AdS 2×S 2 sigma模型有关。在AdS 3×S 3和AdS 5×S 5情况下,预期会有类似的结果。

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