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Graviton and gauge boson propagators in AdS(d+1)

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arxiv hep-th/9902042 v1 pith:ZH5RQ7NN submitted 1999-02-04 hep-th gr-qc

Eric D'Hoker , Daniel Z. Freedman , Samir D. Mathur , Alec Matusis , Leonardo Rastelli This is my paper · ORCID
classification hep-thgr-qc
keywords gaugepropagatorsgravitoninvariantleadsmethodmethodsparts
verification ladder T0 review T1 audit T2 compute T3 formal
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We construct the gauge field and graviton propagators in Euclidean AdS(d+1) space-time by two different methods. In the first method the gauge invariant Maxwell or linearized Ricci operator is applied directly to bitensor ansatze for the propagators which reflect their gauge structure. This leads to a rapid determination of the physical part of the propagators in terms of elementary functions. The second method is a more traditional approach using covariant gauge fixing which leads to a solution for both physical and gauge parts of the propagators. The gauge invariant parts agree in both methods.

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Cited by 5 Pith papers

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