Derivative of the Lie-group exponential #
Let center = extChartAt I 1 1 and let F be the tangent-space exponential written in the
extended chart at the identity. Smoothness of the exponential makes F differentiable at zero.
Along each line t ↦ t • v, the scaling law identifies F with the coordinate expression of
the canonical integral curve generated by v. Its initial velocity is v, so F has derivative
the identity at zero; equivalently, F(v) = F(0) + v + o(‖v‖). The same integral-curve
calculation supplies reusable chain rules for functions along translated exponential lines.
Main results #
hasFDerivAt_extChartAt_mulInvariantExp_zero: in model-space identity coordinates, the tangent-space exponential has derivative the identity at zero.hasFDerivAt_extChartAt_lieExp_zero: the identity-chart derivative of the derivation-based exponential is the canonical linear isometry to the model space.hasFDerivAt_extChartAt_mulInvariantExp_smul_mul_mulInvariantExp_smul_zero: two exponential lines multiplied together have initial coordinate derivativeX + Y.contMDiff_mulInvariantExp_smul: an exponential line is smooth.contMDiff_mulInvariantExp_smul_mul_mul_mulInvariantExp_smul: two exponential lines multiplied around a fixed group element give a smooth two-parameter map.hasMFDerivAt_mulInvariantExp_smul_zero: an exponential line has its generator as initial velocity.hasMFDerivAt_mulInvariantExp_smul: at every time, an exponential line's velocity is its generating left-invariant vector field at the current point.HasMFDerivAt.hasDerivAt_comp_mulInvariantExp_smul_zero: the chain rule along an exponential line at zero.HasMFDerivAt.hasDerivAt_comp_mul_mulInvariantExp_smul_zero: the chain rule after left translation at zero.HasMFDerivAt.hasDerivAt_comp_mulInvariantExp_smul_mul_zero: the chain rule after right translation at zero.LeftInvariantDerivation.hasDerivAt_apply_mul_lieExp_smul: a left-invariant derivationXis the derivative along the exponential linest ↦ g * lieExp (t • X)it generates.
The exponential line generated by X is smooth.
Two exponential lines multiplied around a fixed group element give a smooth two-parameter map.
At time t, an exponential line has velocity the left-invariant vector field generated by X,
evaluated at the point mulInvariantExp (t • X) reached by the line.
The exponential line generated by X has initial velocity X.
Differentiating a function that is manifold-differentiable at the identity along an exponential line gives its directional derivative there.
Differentiating a function after left multiplication along an exponential line gives its left-invariant directional derivative.
Differentiating a function after right multiplication along an exponential line gives its right-invariant directional derivative.
In model-space identity coordinates, the tangent-space exponential has derivative the identity at zero.
In identity-chart coordinates, the derivative of the derivation-based Lie exponential at zero is the canonical linear isometry from left-invariant derivations to the model space.
In identity-chart coordinates, the product of the exponential lines generated by X and
Y has initial derivative X + Y.
Derivatives along exponential lines of left-invariant derivations #
A left-invariant derivation differentiates along its exponential lines. The derivative of
t ↦ f (g * lieExp (t • X)) at every time t is X f at the current point.
The derivative of f along the exponential lines of X is X f along the same lines.