词条 | Draft:Lie's formula |
释义 |
Lie's formula, due to Sophus Lie (1888), says: if {{math|p}} is a point on a real or complex analytic manifold {{math|M}}, {{math|X}} is a analytic vector field, {{math|φ}} an analytic function, then where on the right X is viewed as a a first order differential operator operating on {{math|φ}}. In other words, it gives the Taylor series of {{math|φ}} along one-parameter subgroup. Here {{math|X}} is an analytic vector field, and {{math|exp}} is the flow of {{math|X}}, and {{math|τ}} is the "time" of the flow. Its proof depends on {{math|φ}} having a Taylor series. In a smooth manifold setting, the exponential mapping is simply defined to be the time one flow of a (left invariant) smooth vector field without the strong motivational point of the power series for its name. On the left hand side, is, for each {{math|τ ∈ R}}, a bi-analytic bijection (the analytic counterpart of diffeomorphism) from the analytic manifold (the Lie group) to itself. Thus is a new point on the manifold. When {{math|τ}} varies ({{math|p}} fixed), an integral curve of {{math|X}} is obtained. With {{math|p}} = the identity, can be considered as a one-parameter subgroup as {{math|τ}} varies over all {{math|R}} (provided {{math|X}} is in the Lie algebra). All one-parameter subgroups of the Lie group are expressible as such for some {{math|X}} in the Lie algebra (the left-invariant vector fields ≃ tangent space at the identity). On the right hand side, {{math|X}} is to be thought of as . Every {{math|X}} in the Lie algebra can canonically be associated with such a differential operator on the whole Lie group. This extends the concept of a Taylor series globally and in a coordinate-independent way. j functionIt is the Jacobian of the exponential map. See also: Kirillov's character formula. |
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