Curvature under a conformal change of metric #
Let g be a Riemannian metric on M and f a positive function, and let ĝ = f g be the
conformally rescaled metric Bundle.ContMDiffRiemannianMetric.rescale. The Levi-Civita
connections of the two metrics differ by the conformal connection tensor
A(Y, X) = (2 f)⁻¹ (df(X) Y + df(Y) X - g(X, Y) grad_g f)
(TauCeti.Manifold.conformalConnectionTensor), and this file computes the curvature of ĝ
from that of g:
R^ĝ(X, Y) Z = R^g(X, Y) Z + (∇_X A)(Z, Y) - (∇_Y A)(Z, X) + A(A(Z, Y), X) - A(A(Z, X), Y),
where ∇ is the Levi-Civita connection of g and
(∇_X A)(Z, Y) = ∇_X (A(Z, Y)) - A(∇_X Z, Y) - A(Z, ∇_X Y). Writing f = e^(2φ), the tensor
is A(Y, X) = dφ(X) Y + dφ(Y) X - g(X, Y) grad_g φ, and this is the classical transformation law
of the Riemann curvature under the conformal change e^(2φ) g.
The identity holds at a point x for a Cⁿ metric with 1 ≤ n, and with the Levi-Civita
connection of g replaced by any connection that is Levi-Civita for g. The conformal factor f
is assumed Cⁿ on all of M and the vector field Z differentiable on all of M; the remaining
hypotheses are differentiability at x of X, Y, ∇_X Z, ∇_Y Z, A(Z, X) and A(Z, Y).
For a smooth metric, a smooth conformal factor and smooth vector fields all the hypotheses hold.
As for the conformal change of the Levi-Civita connection
(Bundle.ContMDiffRiemannianMetric.leviCivitaConnection_rescale_apply), connections do not depend
on a metric, so each metric is installed in turn as the RiemannianBundle instance of the tangent
bundle of M and the connections are compared directly on M.
For a smooth metric and a smooth conformal factor f = e^(2φ), the difference of the two
curvatures is a tensor built from the Hessian Hess φ, the differential dφ and the gradient
grad φ, so it can be evaluated pointwise and contracted. The factor is given as a smooth
positive function f together with a function φ satisfying f = e^(2φ); such a φ is
automatically smooth. With n the dimension, Δ = div grad
the Laplace–Beltrami operator of g and R(u, v) w = ∇_u ∇_v w - ∇_v ∇_u w - ∇_[u,v] w, the
contractions are the classical formulas
Ric^ĝ = Ric^g - (n - 2) (Hess φ - dφ ⊗ dφ) + (-Δφ - (n - 2) |dφ|²) g,
Scal^ĝ = e^(-2φ) (Scal^g - 2 (n - 1) Δφ - (n - 1) (n - 2) |dφ|²).
The scalar formula is the input from which the conformal Laplacian of the Yamabe problem arises.
In dimension two it becomes Scal^ĝ = e^(-2φ) (Scal^g - 2 Δφ), the curvature equation of
conformal metrics on surfaces.
In dimension n ≥ 3 the Ricci and scalar formulas combine into the transformation law of the
Schouten tensor P = (Ric - Scal g / (2 (n - 1))) / (n - 2),
P^ĝ = P^g - Hess φ + dφ ⊗ dφ - (|dφ|² / 2) g,
Since the fully covariant curvature tensor of ĝ is e^(2φ) (Rm^g - T ⊙ g), with ⊙ the
Kulkarni–Nomizu product and T = Hess φ - dφ ⊗ dφ + (|dφ|² / 2) g the same correction, the Weyl
tensor W = Rm - P ⊙ g satisfies W^ĝ = f W^g for ĝ = f g, away from dimension 2.
Equivalently, the Weyl tensor of type (1, 3) is a conformal invariant; in particular its
vanishing depends only on the conformal class. This is the conformal invariance used in the
characterization of local conformal flatness by the Weyl tensor.
Differentiating the Schouten law gives the transformation law of the Cotton tensor
C(X, Y, Z) = (∇_Z P)(X, Y) - (∇_Y P)(X, Z): for ĝ = e^(2φ) g, away from dimension 2,
C^ĝ(X, Y, Z) = C^g(X, Y, Z) + W^g(Y, Z, grad φ, X).
The third derivatives of φ cancel by the Ricci identity for the Hessian
(TauCeti.Manifold.mvfderiv_hessian_sub_swap), the change of connection contributes the
Kulkarni–Nomizu part of the curvature, and only the Weyl tensor survives. In dimension 3 the
Weyl tensor vanishes, so the Cotton tensor is a conformal invariant there; this is the
conformal invariance used in the three-dimensional characterization of local conformal flatness.
Main results #
Bundle.ContMDiffRiemannianMetric.curvatureOperator_leviCivitaConnection_rescale: the curvature off gin terms of a Levi-Civita connection ofgand the conformal connection tensor off.Bundle.ContMDiffRiemannianMetric.curvatureOperator_leviCivitaConnection_rescale_of_contMDiff: the same identity for a smooth metric, a smooth conformal factor and smooth vector fields.Bundle.ContMDiffRiemannianMetric.curvatureTensor_leviCivitaConnection_rescale: the pointwise curvature tensor ofe^(2φ) gin terms of that ofg,Hess φ,dφandgrad φ.Bundle.ContMDiffRiemannianMetric.ricciTensor_leviCivitaConnection_rescale: the Ricci tensor ofe^(2φ) g.Bundle.ContMDiffRiemannianMetric.scalarCurvature_rescale: the scalar curvature ofe^(2φ) g.Bundle.ContMDiffRiemannianMetric.scalarCurvature_rescale_of_finrank_eq_two: on a surface,Scal^(e^(2φ) g) = e^(-2φ) (Scal^g - 2 Δφ).Bundle.ContMDiffRiemannianMetric.scalarCurvature_rescale_eq_iff_of_finrank_eq_two: on a surface,e^(2φ) ghas scalar curvaturecexactly when-Δφ + Scal^g / 2 = (c / 2) e^(2φ).Bundle.ContMDiffRiemannianMetric.schoutenTensor_leviCivitaConnection_rescale: the Schouten tensor ofe^(2φ) g.Bundle.ContMDiffRiemannianMetric.weylTensor_leviCivitaConnection_rescale: the Weyl tensor off gisftimes that ofg.Bundle.ContMDiffRiemannianMetric.weylTensor_leviCivitaConnection_rescale_eq_zero_iff: the Weyl tensor off gvanishes at a point exactly when that ofgdoes.Bundle.ContMDiffRiemannianMetric.cottonTensor_leviCivitaConnection_rescale: the Cotton tensor ofe^(2φ) gis that ofgplus the Weyl tensor ofgcontracted withgrad φ.Bundle.ContMDiffRiemannianMetric.cottonTensor_leviCivitaConnection_rescale_of_finrank_eq_three: in dimension3the Cotton tensor off gequals that ofg.
References #
- A. L. Besse, Einstein Manifolds, Springer (1987), Sections 1.G and 1.J.
- J. M. Lee, Introduction to Riemannian Manifolds, 2nd ed., Springer GTM 176 (2018), Chapter 7 (curvature of conformally related metrics).
- J. M. Lee and T. H. Parker, The Yamabe problem, Bull. Amer. Math. Soc. 17 (1987), 37–91, Section 2.
Curvature under conformal change. Let ∇ be a Levi-Civita connection of a C¹ metric g
and A the conformal connection tensor of a positive function f. Then the curvature of the
Levi-Civita connection of f g is
R^(f g)(X, Y) Z = R^∇(X, Y) Z + (∇_X A)(Z, Y) - (∇_Y A)(Z, X) + A(A(Z, Y), X) - A(A(Z, X), Y),
with (∇_X A)(Z, Y) = ∇_X (A(Z, Y)) - A(∇_X Z, Y) - A(Z, ∇_X Y). The metric g and the
function f are assumed Cⁿ on all of M for some 1 ≤ n, and Z differentiable on all of M;
the remaining hypotheses are differentiability at x of X, Y, ∇_X Z, ∇_Y Z, A(Z, X) and
A(Z, Y).
Curvature under conformal change, for a smooth metric g, a smooth positive function f
and smooth vector fields. With ∇ the Levi-Civita connection of g and A the conformal
connection tensor of f, the curvature of the Levi-Civita connection of f g is
R^(f g)(X, Y) Z = R^g(X, Y) Z + (∇_X A)(Z, Y) - (∇_Y A)(Z, X) + A(A(Z, Y), X) - A(A(Z, X), Y),
with (∇_X A)(Z, Y) = ∇_X (A(Z, Y)) - A(∇_X Z, Y) - A(Z, ∇_X Y).
Curvature tensor under conformal change. Let g be a smooth metric and f = e^(2φ) a
smooth positive function. With Hess φ, ∇ and grad φ taken for g, the curvature tensor of
f g at x is
R^(f g)(u, v) w = R^g(u, v) w + Hess φ(u, w) v - Hess φ(v, w) u + g(u, w) ∇_v grad φ
- g(v, w) ∇_u grad φ + dφ(v) dφ(w) u - dφ(u) dφ(w) v + (dφ(u) g(v, w) - dφ(v) g(u, w)) grad φ
- |dφ|² (g(v, w) u - g(u, w) v).
Ricci tensor under conformal change. Let g be a smooth metric on a manifold of
dimension n and f = e^(2φ) a smooth positive function. Then
Ric^(f g) = Ric^g - (n - 2) (Hess φ - dφ ⊗ dφ) + (-Δφ - (n - 2) |dφ|²) g, where Hess φ,
Δφ = div grad φ and |dφ| are taken for g.
Scalar curvature under conformal change. Let g be a smooth metric on a manifold of
dimension n and f = e^(2φ) a smooth positive function. Then
Scal^(f g) = f⁻¹ (Scal^g - 2 (n - 1) Δφ - (n - 1) (n - 2) |dφ|²), where Δφ = div grad φ and
|dφ| are taken for g.
Scalar curvature under conformal change on a surface. Let g be a smooth metric on a
surface and f = e^(2φ) a smooth positive function. Then
Scal^(f g) = f⁻¹ (Scal^g - 2 Δφ), where Δφ = div grad φ is taken for g.
The prescribed curvature equation on a surface. Let g be a smooth metric on a surface
and f = e^(2φ) a smooth positive function. Then e^(2φ) g has scalar curvature c at x
exactly when -Δφ + Scal^g / 2 = (c / 2) e^(2φ) there, where Δφ = div grad φ is taken for
g. Since the scalar curvature of a surface is twice its Gaussian curvature, for c = -2 this is
the equation Δ⁺φ + K + e^(2φ) = 0 for a metric of Gaussian curvature -1, where
Δ⁺ = -div grad and K = Scal^g / 2.
Schouten tensor under conformal change. Let g be a smooth metric on a manifold of
dimension n ≥ 3 and f = e^(2φ) a smooth positive function. Then the Schouten tensor of f g is
P^(f g) = P^g - Hess φ + dφ ⊗ dφ - (|dφ|² / 2) g, where Hess φ and |dφ| are taken for g.
Weyl tensor under conformal change. Away from dimension 2, the fully covariant Weyl
tensor of a conformally rescaled smooth metric f g is f times that of g:
W^(f g)(u, v, w, z) = f W^g(u, v, w, z). Equivalently, the Weyl tensor of type (1, 3) is
conformally invariant.
Away from dimension 2, the Weyl tensor of a conformally rescaled smooth metric f g vanishes
at a point exactly when that of g does.
Cotton tensor under conformal change. Let g be a smooth metric on a manifold of
dimension n ≠ 2 and f = e^(2φ) a smooth positive function. Then the Cotton tensor of f g is
C^(f g)(u, v, w) = C^g(u, v, w) + W^g(v, w, grad φ, u), where W^g is the Weyl tensor of g
and grad φ is taken for g.
The Cotton tensor is conformally invariant in dimension 3. On a manifold of dimension
3, where the Weyl tensor vanishes, the Cotton tensor of a conformally rescaled smooth metric
f g equals that of g.