Documentation

TauCeti.Geometry.Manifold.VectorBundle.Riemannian.Cotangent

The norm of covectors on a Riemannian manifold #

A Riemannian metric g on a finite-dimensional manifold M induces a norm on each cotangent space T*ₓM: the operator norm of a covector p for the norm of g on TₓM, which is the norm of its Riesz dual, ‖p‖² = p(p♯). This file studies the function z ↦ ‖z.2‖ on the total space of the cotangent bundle T*M = TauCeti.CotangentBundle I M.

In the chart-local frame (eᵢ) of TM at a point, ‖p‖² = Σᵢⱼ gⁱʲ p(eᵢ) p(eⱼ), where gⁱʲ is the inverse Gram matrix of the frame. The components p(eᵢ) are the bundle coordinates of p, so this formula shows that z ↦ ‖z.2‖² is C^n on T*M when g is (TauCeti.CotangentBundle.contMDiff_norm_snd_sq). Consequently the norm itself is continuous, and C^n away from the zero section.

Along the fibre ray t ↦ t • z the norm is t ↦ |t| ‖z.2‖, so its differential does not vanish off the zero section: every nonzero value is a regular value of z ↦ ‖z.2‖ (TauCeti.CotangentBundle.isRegularValue_norm_snd). Its levels are the cosphere bundles of g, which are therefore smooth hypersurfaces of T*M when M has no boundary.

Main results #

References #

The squared norm of covectors is smooth. For a C^n Riemannian metric, the function z ↦ ‖z.2‖² on the cotangent bundle is C^n.

Off the zero section, the norm of covectors is as smooth as the metric.

The norm of covectors is continuous on the cotangent bundle of a manifold with a continuous Riemannian metric.

The norm of covectors along the Euler vector field. At a covector z other than zero, the differential of z ↦ ‖z.2‖ sends the Euler vector field p ∂_p to ‖z.2‖: along the fibre ray t ↦ t • z the norm is t ↦ |t| ‖z.2‖.

Covectors other than zero are regular points of the norm. Every covector z with z.2 ≠ 0 is a regular point of z ↦ ‖z.2‖.

Every nonzero value is a regular value of the norm of covectors. Its levels are the cosphere bundles of the metric.