In differential geometry, a Lie group action is a group action adapted to the smooth setting: G is a Lie group, M is a smooth manifold, and the action map is differentiable.
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Let be a (left) group action of a Lie group G on a smooth manifold M; it is called a Lie group action (or smooth action) if the map is differentiable. Equivalently, a Lie group action of G on M consists of a Lie group homomorphism . A smooth manifold endowed with a Lie group action is also called a G-manifold.
The fact that the action map is smooth has a couple of immediate consequences:
the stabilizers of the group action are closed, thus are Lie subgroups of G
the orbits of the group action are immersed submanifolds.
Forgetting the smooth structure, a Lie group action is a particular case of a continuous group action.
For every Lie group G, the following are Lie group actions:
the trivial action of G on any manifold
the action of G on itself by left multiplication, right multiplication or conjugation
the action of any Lie subgroup on G by left multiplication, right multiplication or conjugation
the adjoint action of G on its Lie algebra .
Other examples of Lie group actions include:
the action of on M given by the flow of any complete vector field
the actions of the general linear group and of its Lie subgroups on by matrix multiplication
more generally, any Lie group representation on a vector space
any Hamiltonian group action on a symplectic manifold
the transitive action underlying any homogeneous space
more generally, the group action underlying any principal bundle
Following the spirit of the Lie group-Lie algebra correspondence, Lie group actions can also be studied from the infinitesimal point of view. Indeed, any Lie group action induces an infinitesimal Lie algebra action on M, i.e. a Lie algebra homomorphism . Intuitively, this is obtained by differentiating at the identity the Lie group homomorphism , and interpreting the set of vector fields as the Lie algebra of the (infinite-dimensional) Lie group .
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In mathematics, a Lie groupoid is a groupoid where the set of s and the set of morphisms are both manifolds, all the operations (source and target, composition, identity-assigning map and inversion) are smooth, and the source and target operations are submersions. A Lie groupoid can thus be thought of as a "many-object generalization" of a Lie group, just as a groupoid is a many-object generalization of a group. Accordingly, while Lie groups provide a natural model for (classical) continuous symmetries, Lie groupoids are often used as model for (and arise from) generalised, point-dependent symmetries.
En topologie, de manière informelle, un fibré principal sur un espace topologique X est un espace ressemblant localement à un produit de X par un groupe topologique. En particulier, un fibré principal est un espace fibré, mais c'est bien plus encore. Il est muni d'un groupe, le groupe structural, décrivant la manière dont les trivialisations locales se recollent entre elles. La théorie des fibrés principaux recouvre la théorie des fibrés vectoriels, de leurs orientations, de leurs structures riemanniennes, de leurs structures symplectiques, etc.
The purpose of this paper is to generalize the (Poisson) Optimal Reduction Theorem in Ortega and Ratiu [Momentum Maps and Hamiltonian Reduction. Progress in Mathematics 222. Boston, MA: Birkhauser. xxxiv, 497pp., 2004] to general proper Lie group actions o ...
In this article, motivated by the study of symplectic structures on manifolds with boundary and the systematic study of b-symplectic manifolds started in Guillemin, Miranda, and Pires Adv. Math. 264 (2014), 864-896, we prove a slice theorem for Lie group a ...
In this paper, the differential geometry of the novel hierarchical Tucker format for tensors is derived. The set HT,k of tensors with fixed tree T and hierarchical rank k is shown to be a smooth quotient manifold, namely the set of orbits of a Lie group ac ...