2014
DOI: 10.48550/arxiv.1412.7559
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An introduction to conformal geometry and tractor calculus, with a view to applications in general relativity

Abstract: The following are expanded lecture notes for the course of eight one hour lectures given by the second author at the 2014 summer school Asymptotic Analysis in General Relativity held in Grenoble by the Institut Fourier. The first four lectures deal with conformal geometry and the conformal tractor calculus, taking as primary motivation the search for conformally invariant tensors and diffrerential operators. The final four lectures apply the conformal tractor calculus to the study of conformally compactified g… Show more

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Cited by 12 publications
(25 citation statements)
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“…A second motivation for our study is that this general setting allows us to study the extrinsic conformal geometry of the boundary geometry. Mathematically, our results are part of a general program to understand conformal hypersurface geometry [GW15] (see [CG15] for an overview), and to develop the calculus for integrated conformal hypersurface invariants begun in [GGHW15]. Indeed, we wish to initiate a new approach to geometric invariant theory based on holographic renormalization.…”
Section: Introductionmentioning
confidence: 99%
“…A second motivation for our study is that this general setting allows us to study the extrinsic conformal geometry of the boundary geometry. Mathematically, our results are part of a general program to understand conformal hypersurface geometry [GW15] (see [CG15] for an overview), and to develop the calculus for integrated conformal hypersurface invariants begun in [GGHW15]. Indeed, we wish to initiate a new approach to geometric invariant theory based on holographic renormalization.…”
Section: Introductionmentioning
confidence: 99%
“…The above flat model for conformal geometry was generalized in [10] by Fefferman and Graham who replaced M d,2 by a d + 2 dimensional manifold equipped with a metric which admits a hypersurface orthogonal homothety. Note that there is a natural interpretation of this picture as curved Cartan geometry; moreover the Cartan approach naturally leads to a Weyl covariant differential calculus, known as tractor calculus, originally constructed in [11] (see also [12,13] for a physics oriented review) and then generalized to all parabolic geometries in [14]. It can be understood as the equivalent of the superfield formalism for conformal invariance.…”
Section: Introductionmentioning
confidence: 99%
“…Let us call defining densities that obey Equation (3.6) unit. Then from Proposition 3.3 and reference [4] (see also [25,10]) we have the following result.…”
Section: Scanned With Camscannermentioning
confidence: 91%
“…where Φ indicates any tensor product of tractor and conformal density bundles. In a self-explanatory matrix notation (see [10])…”
Section: Scanned With Camscannermentioning
confidence: 99%
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