1991
DOI: 10.1090/s0002-9947-1991-0991959-1
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The existence of generalized isothermal coordinates for higher-dimensional Riemannian manifolds

Abstract: We shall show that, for any given point p on a Riemannian manifold (M, g), there is a pointwise conformai metric g = g in which thê-geodesic sphere centered at p with radius r has constant mean curvature 1/r for all sufficiently small r. Furthermore, the exponential map of g at p is a measure preserving map in a small ball around p .

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Cited by 20 publications
(23 citation statements)
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“…Let (M, g) be a smooth Riemannian manifold of dimension n ≥ 5, and P g be the Paneitz operator on M . For any pointX ∈ M , it was proved in [30], together with some improvement in [7] and [16], that there exists a positive smooth function κ (with control) on M such that the conformal metricg = κ We refer such coordinates as conformal normal coordinates. Notice that detg = 1 + O(|x| N ) will be enough for our use if N is sufficiently large.…”
Section: Paneitz Operator In Conformal Normal Coordinatesmentioning
confidence: 99%
“…Let (M, g) be a smooth Riemannian manifold of dimension n ≥ 5, and P g be the Paneitz operator on M . For any pointX ∈ M , it was proved in [30], together with some improvement in [7] and [16], that there exists a positive smooth function κ (with control) on M such that the conformal metricg = κ We refer such coordinates as conformal normal coordinates. Notice that detg = 1 + O(|x| N ) will be enough for our use if N is sufficiently large.…”
Section: Paneitz Operator In Conformal Normal Coordinatesmentioning
confidence: 99%
“…Here and in the sequel, the exponential map exp ξ is always intended with respect to the metric g ξ . We refer to Lee-Parker [27] for a proof of the existence of conformal normal coordinates of any finite order, see also the later proofs by Cao [11] and Günther [22] of the existence of conformal normal coordinates which are volume preserving near a given point (with no remainder term in (2.4)). For any ξ ∈ M, we let Λ ξ be the smooth positive function in M such that g ξ = Λ 2 * −2 ξ g. In both cases (locally conformally flat or not), the metric g ξ can be chosen smooth with respect to ξ and such that Λ ξ (ξ) = 1 and ∇Λ ξ (ξ) = 0.…”
Section: Scheme Of the Proofmentioning
confidence: 99%
“…L g is referred to as the conformal Laplacian, and the boundary value problem (2.1) is conformally invariant (see proposition A.2). In conformal normal coordinates (see [27,41,11]) centered at a point p, we write g(x) = exp(h(x)), where h is a smooth function taking values in the space of symmetric n × n matrices. From standard properties of conformal normal coordinates it then follows that x j h ij (x) = 0, and tr h ij (x) = O(r N ), where r = dist g (x, p) and N is arbitrarily large.…”
Section: Setting Notation and Basic Definitionsmentioning
confidence: 99%