Lifts an action of a finite-dimensional Lie algebra on a manifold to a Lie group action
In differential geometry, the Lie–Palais theorem states that an action of a finite-dimensional Lie algebra on a smoothcompact manifold can be lifted to an action of a finite-dimensional Lie group. For manifolds with boundary the action must preserve the boundary; in other words, the vector fields on the boundary must be tangent to the boundary. Palais (1957) proved it as a global form of an earlier local theorem due to Sophus Lie.
The example of the vector fieldd/dx on the open unit interval shows that the result is false for non-compact manifolds.
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: the Lie algebra is all vector fields f(x, y) ∂/∂x + g(x, y) ∂/∂y acting on the torus R2/Z2 such that g(x, y) = 0 for 0 ≤ x ≤ 1/2. This Lie algebra is not the Lie algebra of any group. 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