Weyl–Schouten on a model space #
For an arbitrary smooth Riemannian metric on a finite-dimensional real normed space, vanishing
Weyl and Cotton tensors near a point give a positive smooth conformal factor making the metric
flat near that point. The exponent φ can have any prescribed value and gradient at
the point. This uses the local solutions of the conformal flattening equation from
TauCeti.Manifold.exists_eventually_hessian_eq_model_space and the curvature decomposition into
Weyl and Schouten tensors.
Consequently a smooth metric on a model space of dimension at least four is locally conformally
flat if and only if its Weyl tensor vanishes. In dimension three the corresponding criterion is
vanishing Cotton tensor: Weyl vanishes identically in that dimension. In higher dimensions the
Cotton condition follows from the divergence identity div W = (dim M - 3) C.
These statements concern arbitrary variable metrics on the model space, rather than only the Euclidean metric. Local conformal flatness here means existence of a flat conformal rescaling; no Euclidean coordinate isometry is assumed.
References #
- A. L. Besse, Einstein Manifolds, Springer (1987), Section 1.G.
- J. M. Lee and T. H. Parker, The Yamabe problem, Bull. Amer. Math. Soc. 17 (1987), Section 2.
Where Weyl and Cotton vanish, a smooth metric on a model space has a flat conformal
rescaling e^(2φ) g near the point, with arbitrary prescribed value and gradient of φ.
A smooth metric on a model space of dimension at least three is locally conformally flat exactly when its Weyl and Cotton tensors both vanish.
Weyl–Schouten in dimension at least four, on a model space. An arbitrary smooth Riemannian metric is locally conformally flat if and only if its Weyl tensor vanishes.
Weyl–Schouten in dimension three, on a model space. An arbitrary smooth Riemannian metric is locally conformally flat if and only if its Cotton tensor vanishes.