Documentation

TauCeti.Geometry.Lie.IntegralCurve

Integral curves of invariant vector fields #

Left-invariant vector fields on real Lie groups modeled on complete spaces are complete. Local integral curves around the identity can be translated to give a uniform existence interval around every point, after which Mathlib's uniform-time theorem produces global integral curves.

Main results #

References #

Left translation preserves integral curves of a left-invariant vector field.

Left translation preserves global integral curves of a left-invariant vector field.

Every left-invariant vector field on a real Lie group modeled on a complete space has a global integral curve through every point.

Every left-invariant vector field on a real Lie group modeled on a complete space has a unique global integral curve through every point.

noncomputable def mulInvariantIntegralCurve {E : Type u_1} [NormedAddCommGroup E] [NormedSpace ℝ E] {H : Type u_2} [TopologicalSpace H] {I : ModelWithCorners ℝ E H} {G : Type u_3} [TopologicalSpace G] [ChartedSpace H G] [Group G] [CompleteSpace E] [LieGroup I (minSmoothness ℝ 3) G] [T2Space G] [BoundarylessManifold I G] (v : GroupLieAlgebra I G) (x : G) :
ℝ → G

The unique global integral curve of a left-invariant vector field through a given point.

Instances For
    @[simp]

    The canonical invariant integral curve starts at its specified point.

    The canonical invariant curve is a global integral curve of its left-invariant vector field.

    In the extended chart at the identity, the canonical invariant curve through the identity has initial velocity equal to its generator.

    The canonical integral curve of an invariant vector field on a smooth Lie group is smooth.

    theorem eq_mulInvariantIntegralCurve {E : Type u_1} [NormedAddCommGroup E] [NormedSpace ℝ E] {H : Type u_2} [TopologicalSpace H] {I : ModelWithCorners ℝ E H} {G : Type u_3} [TopologicalSpace G] [ChartedSpace H G] [Group G] [CompleteSpace E] [LieGroup I (minSmoothness ℝ 3) G] [T2Space G] [BoundarylessManifold I G] (v : GroupLieAlgebra I G) (x : G) {γ : ℝ → G} (hγ0 : γ 0 = x) (hγ : IsMIntegralCurve γ (mulInvariantVectorField v)) :

    Any global integral curve of a left-invariant vector field is the canonical one determined by its value at zero.

    The canonical invariant integral curve through x is the left translate by x of the canonical curve through the identity.

    @[simp]

    The canonical invariant curve through the identity satisfies the one-parameter subgroup law.

    Scaling an invariant vector field rescales time along its canonical integral curves.

    The canonical invariant curve through the identity, bundled as a continuous one-parameter subgroup.

    Instances For
      @[simp]

      Evaluating the invariant one-parameter subgroup at time t recovers the canonical integral curve through the identity.

      The one-parameter subgroup generated by an invariant vector field is smooth in its additive real parameter.