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I need help calculating the exponential map of a general vector.
Definition of the exponential map
For a Lie group G with Lie algebra \mathfrak{g}, and a vector X \in \mathfrak{g} \equiv T_eG, let \hat{X} be the corresponding left-invariant vector field. Then let \gamma_X(t) be the maximal integral curve of \hat{X} such that \gamma_X(0)=e. Then the exponential map \mbox{exp}:\mathfrak{g} \to G is \mbox{exp}(A) = \gamma_A(1).
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It can be shown that the exponential map when A is a matrix is just the 'exponential taylor series' in matrix form.
However, how do you actually compute the exponential map for a general vector that isn't a matrix?
Say, for example, we have the Lie group \mathbb{R}^2 - \lbrace (0,0)\rbrace with binary operation (a,b) *(c,d) = (ac-bd,ad+bc), with identity (1,0) and basis \left(\frac{\partial}{\partial x}\bigg|_{(1,0)},\frac{\partial}{\partial y}\bigg|_{(1,0)}\right). What steps are required to compute \mbox{exp}\left(\frac{\partial}{\partial x}\bigg|_{(1,0)}\right) here?
Definition of the exponential map
For a Lie group G with Lie algebra \mathfrak{g}, and a vector X \in \mathfrak{g} \equiv T_eG, let \hat{X} be the corresponding left-invariant vector field. Then let \gamma_X(t) be the maximal integral curve of \hat{X} such that \gamma_X(0)=e. Then the exponential map \mbox{exp}:\mathfrak{g} \to G is \mbox{exp}(A) = \gamma_A(1).
_______________________________________________________________________
It can be shown that the exponential map when A is a matrix is just the 'exponential taylor series' in matrix form.
However, how do you actually compute the exponential map for a general vector that isn't a matrix?
Say, for example, we have the Lie group \mathbb{R}^2 - \lbrace (0,0)\rbrace with binary operation (a,b) *(c,d) = (ac-bd,ad+bc), with identity (1,0) and basis \left(\frac{\partial}{\partial x}\bigg|_{(1,0)},\frac{\partial}{\partial y}\bigg|_{(1,0)}\right). What steps are required to compute \mbox{exp}\left(\frac{\partial}{\partial x}\bigg|_{(1,0)}\right) here?