The infinitesimal adjoint action #
This file identifies the derivative of the tangent-space adjoint action at the identity with Mathlib's Lie-algebra adjoint map. This is the geometric prerequisite for transporting the result to the derivation-valued group adjoint representation.
This advances Deliverable A, Layer 1 of
TauCetiRoadmap/RepresentationTheory/LieGroups/README.md.
Main results #
TauCeti.Lie.hasDerivAt_tangentAd_mulInvariantExp_smul_apply_zero: att = 0, the derivative of the tangent adjoint action along the exponential line ofXis the Lie bracket.TauCeti.Lie.mvfderiv_tangentAd_apply_one: the differential of the tangent adjoint action at the identity is the Lie-algebra adjoint action.
References #
- Lie groups and the Lie algebra correspondence roadmap, Deliverable A, Layer 1, "The infinitesimal adjoint".
- The two-parameter Clairaut argument adapts
TauCeti.Lie.mvfderiv_mulRightInvariantVectorField_mulInvariantVectorField_commute; its mixed-partial step usesTauCeti.Analysis.Calculus.ParametricFDeriv, which in turn adapts Sébastien Gouëzel'sContDiffAt.isSymmSndFDerivAt.
At t = 0, the derivative of t ↦ tangentAd (mulInvariantExp (t • X)) Y along the
exponential line of X is ⁅X, Y⁆.
GroupLieAlgebra I G reduces definitionally to the model E; the show E from ascriptions expose
that model to the normed-space derivative API.
The derivative at 1 of g ↦ tangentAd g Y, in the direction X, is the Lie-algebra
adjoint LieAlgebra.ad ℝ _ X Y.
GroupLieAlgebra I G reduces definitionally to the model E; the show E from ascriptions expose
that model to the manifold derivative API.