The Euler vector field of a vector bundle #
The fibres of a vector bundle V → B are vector spaces, so every vector z in the total space
lies on the line t ↦ t • z through the origin of its fibre. The velocity of that line at
t = 1 is the Euler vector field (or radial vector field) of the bundle
(TauCeti.vectorBundleEulerField). In a bundle chart with coordinates (x, ξ) it is
ξ ∂_ξ: at z its coordinates are (0, ξ), where ξ is the fibre coordinate of z
(TauCeti.vectorBundleEulerField_eq_trivializationAt). It is vertical, that is, killed by the
derivative of the projection (TauCeti.mfderiv_proj_vectorBundleEulerField), it vanishes along
the zero section (TauCeti.vectorBundleEulerField_zero), and it is smooth
(TauCeti.contMDiff_vectorBundleEulerField). The differential of a map sends it to the velocity of
the image of the line t ↦ t • z (TauCeti.mfderiv_vectorBundleEulerField), so maps between
vector bundles which are linear on fibres preserve Euler vector fields
(TauCeti.mfderiv_vectorBundleEulerField_of_linear).
It is the infinitesimal generator of the fibre dilations z ↦ c • z
(TauCeti.vectorBundleScalarDiffeomorph): on a real vector bundle, the curve t ↦ e^t • z is an
integral curve of the Euler vector field (TauCeti.isMIntegralCurve_vectorBundleEulerField). These
curves are defined for all time, so the Euler vector field is complete
(TauCeti.isCompleteVectorField_vectorBundleEulerField). On a cotangent bundle it is the field
p ∂_p, the Liouville vector field of the canonical symplectic structure.
Main declarations #
TauCeti.vectorBundleEulerField: the Euler vector field.TauCeti.hasMFDerivAt_vectorBundleEulerField: it is the velocity att = 1oft ↦ t • z.TauCeti.mfderiv_vectorBundleEulerField: its image under a differential is the velocity of the image of the linet ↦ t • z.TauCeti.mfderiv_vectorBundleEulerField_of_linear: fibrewise linear maps preserve it.TauCeti.vectorBundleEulerField_eq_trivializationAt: its coordinates in the chart atz.TauCeti.mfderiv_proj_vectorBundleEulerField: it is vertical.TauCeti.contMDiff_vectorBundleEulerField: it is a smooth section of the tangent bundle of the total space.TauCeti.isMIntegralCurve_vectorBundleEulerField: on a real vector bundle, the curvest ↦ e^t • zare integral curves of it.TauCeti.isCompleteVectorField_vectorBundleEulerField: it is complete.
References #
- S. Lang, Fundamentals of Differential Geometry, Graduate Texts in Mathematics 191, Springer, 1999, Chapter IV (sprays, and the dilations of the fibres of a vector bundle).
The Euler vector field of a vector bundle: at a vector z of the total space, the velocity
at t = 1 of the line t ↦ t • z in the fibre of z. In a bundle chart with coordinates (x, ξ)
it is ξ ∂_ξ (TauCeti.vectorBundleEulerField_eq_trivializationAt).
Instances For
Chart formula for the Euler vector field. Read in the chart at z, where tangent vectors
at z are their own coordinates, the Euler vector field at z is (0, ξ), with ξ the fibre
coordinate of z in the trivialization at its base point.
The Euler vector field at z is the velocity at t = 1 of the line t ↦ t • z.
The Euler vector field along a map. The differential at z of a map f sends the Euler
vector field to the velocity at t = 1 of the image under f of the line t ↦ t • z.
Fibrewise linear maps preserve Euler vector fields. A map between the total spaces of two
vector bundles which covers a map g of the bases and is linear on each fibre sends the Euler
vector field to the Euler vector field, at every point where it is differentiable.
The Euler vector field vanishes along the zero section.
The Euler vector field is vertical: the derivative of the bundle projection kills it.
Smoothness of the Euler vector field. The Euler vector field is a C^m section of the
tangent bundle of the total space, for every m.
The flow of the Euler vector field #
The flow of the Euler vector field is fibre dilation. For every vector z of a real vector
bundle, the curve t ↦ e^t • z is an integral curve of the Euler vector field.
The Euler vector field is complete: through every vector z of a real vector bundle, the
fibre dilation t ↦ e^t • z is an integral curve defined for all time.