First-order quantities 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 two metrics live on the
copies TauCeti.WithMetric g and TauCeti.WithMetric ĝ of M, so that each carries its own
RiemannianBundle instance. This file compares the quantities of first order in the metric:
- the inner product:
⟪v, w⟫_ĝ = f ⟪v, w⟫_g; - the inverse metric on arbitrary covectors: raising an index and pairing covectors scale by
f⁻¹, and the covector operator norm scales by1 / √f; - the gradient, through the inverse metric:
grad_ĝ u = f⁻¹ grad_g u, and hence⟪grad_ĝ u, grad_ĝ w⟫_ĝ = f⁻¹ ⟪grad_g u, grad_g w⟫_g; - the chart Gram matrix and its inverse,
G_ĝ = f G_gandG_ĝ⁻¹ = f⁻¹ G_g⁻¹, and the volume density,dV_ĝ = f ^ (n / 2) dV_gin real dimensionn.
Tangent vectors of the copies are compared with tangent vectors of M through the differential of
TauCeti.WithMetric.ofWithMetric, which is the identity of the model space. Covectors on M
are pulled back by that same differential, so each copy carries its own metric norm. Index raising
uses Riemannian.Tensor.rieszDual. The inverse-metric laws hold for Cⁿ metrics and positive
Cⁿ factors, including n = 0.
For the Yamabe problem, f = u ^ (4 / (n - 2)) with u positive, so that
f ^ (n / 2) = u ^ (2 n / (n - 2)).
Main results #
TauCeti.WithMetric.inner_rescale: the inner product of the rescaled metric.TauCeti.WithMetric.mfderiv_ofWithMetric_rieszDual_rescale: raising a covector's index for the rescaled metric multiplies its transported Riesz dual byf⁻¹.TauCeti.WithMetric.apply_rieszDual_rescale: the inverse-metric pairing scales byf⁻¹.TauCeti.WithMetric.norm_sq_covector_rescaleandTauCeti.WithMetric.norm_covector_rescale: the squared covector norm scales byf⁻¹, and the norm by1 / √f.TauCeti.WithMetric.mfderiv_ofWithMetric_mgradient_rescale: the gradient for the rescaled metric isf⁻¹times the gradient forg.TauCeti.WithMetric.inner_mgradient_rescale: the corresponding identity for the pointwise Dirichlet energy density.TauCeti.WithMetric.chartGramMatrix_rescaleandTauCeti.WithMetric.chartInvGramMatrix_rescale: the chart Gram matrix scales byf, and its inverse byf⁻¹.TauCeti.WithMetric.chartVolumeDensity_rescale: the volume density of the rescaled metric isf ^ (n / 2)times that ofg.
References #
- J. M. Lee, Introduction to Riemannian Manifolds, 2nd ed., Springer GTM 176 (2018), Chapter 2 (conformal metrics, dual metric, gradient and volume form).
- J. M. Lee and T. H. Parker, The Yamabe problem, Bull. Amer. Math. Soc. 17 (1987), 37–91, Section 2.
The inner product of the rescaled metric f g is f times that of g.
Raising the index of a covector for f g gives f⁻¹ times its Riesz dual for g,
with both vectors transported to the underlying manifold.
The inverse-metric pairing φ(ψ♯) of two covectors scales by f⁻¹ under g ↦ f g.
The squared operator norm of an arbitrary covector scales by f⁻¹ under g ↦ f g.
The operator norm of a covector for f g is its norm for g divided by √f.
Gradient under conformal change. The gradient of a function for the rescaled metric
f g is f⁻¹ times its gradient for g, both read as tangent vectors of M.
The inner product of two gradients for the rescaled metric f g is f⁻¹ times the inner
product of the gradients for g. With u = w, this is the pointwise Dirichlet energy
density |du|²_{f g} = f⁻¹ |du|²_g.
The chart Gram matrix of the rescaled metric f g is f times that of g.
In chart coordinates, the inverse Gram matrix of f g is f⁻¹ times that of g.
Volume density under conformal change. In real dimension n, the volume density of the
rescaled metric f g in any chart is f ^ (n / 2) times that of g.