Lifts an action of a finite-dimensional Lie algebra on a manifold to a Lie group action
In differential geometry, a field of mathematics, the Lie–Palais theorem is a partial converse to the fact that any smooth action of a Lie group induces an infinitesimal action of its Lie algebra. Palais (1957) proved it as a global form of an earlier local theorem due to Sophus Lie.
If is a manifold with boundary, the statement holds true if the action preserves the boundary; in other words, the vector fields on the boundary must be tangent to the boundary.
Counterexamples
The example of the vector field on the open unit interval shows that the result is false for non-compact manifolds.
Similarly, without the assumption that the Lie algebra is finite-dimensional, the result can be false. Milnor (1984, p. 1048) gives the following example due to Omori: consider the Lie algebra of vector fields of the form acting on the torus such that for . This Lie algebra is not the Lie algebra of any group.
Infinite-dimensional generalization
Pestov (1995) gives an infinite-dimensional generalization of the Lie–Palais theorem for Banach–Lie algebras with finite-dimensional center.
References
Milnor, John Willard (1984), "Remarks on infinite-dimensional Lie groups", Relativity, groups and topology, II (Les Houches, 1983), Amsterdam: North-Holland, pp. 1007–1057, MR0830252 Reprinted in collected works volume 5.
Palais, Richard S. (1957), "A global formulation of the Lie theory of transformation groups", Memoirs of the American Mathematical Society, 22: iii+123, ISBN978-0-8218-1222-8, ISSN0065-9266, MR0121424