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Lie group–Lie algebra correspondence : ウィキペディア英語版
Lie group–Lie algebra correspondence
In mathematics, Lie group–Lie algebra correspondence allows one to study Lie groups, which are geometric objects, in terms of Lie algebras, which are linear objects. In this article, a Lie group refers to a real Lie group. For the complex and ''p''-adic cases, see complex Lie group and ''p''-adic Lie group.
In this article, manifolds (in particular Lie groups) are assumed to be second countable; in particular, they have at most countably many connected components.
== Basics ==
Given a Lie group ''G'', let \operatorname(G) be its associated Lie algebra—the Lie subalgebra of the Lie algebra of vector fields on ''G'' that consists of vector fields ''X'' that are invariant under left translations; that is, for any ''g'', ''h'' in ''G'',
:(dl_g)_h(X_h) = X_
where l_g: G \to G, x \mapsto gx and (dl_g)_h: T_h G \to T_ G is the differential of l_g between tangent spaces.〔In other words, a vector field on ''G'' is left-invariant if it is l_g-related to itself for any ''g'' in ''G''.〕 The left-invariance amounts to the fact that the vector bundle map over ''G''
:\phi: G \times \operatorname(G) \to TG
given by \phi_g(X) = X_g is an isomorphism (note φ makes TG a Lie group). It follows that the canonical map
:\operatorname(G) \to T_e G, \, X \mapsto X_e
is an isomorphism of vector spaces and one usually identifies \operatorname(G) with T_e G. (There is also a third incarnation of \operatorname(G); see "related constructions" below.) In particular, the dimension of ''G'' as a real manifold is the dimension of the vector space \operatorname(G), and \operatorname(G) = \operatorname(G^0) where G^0 is the connected component of the identity element.
If
:f: G \to H
is a Lie group homomorphism, then its differential at the identity element
:df = df_e: \operatorname(G) \to \operatorname(H)
is a Lie algebra homomorphism (brackets go to brackets), which has the following properties:
*\operatorname(\operatorname(f)) = \operatorname(df).〔More generally, if ''H''' is a closed subgroup of ''H'', then \operatorname(f^(H')) = (df)^(\operatorname(H')).
*If the image of ''f'' is closed,〔This requirement cannot be omitted; see also http://math.stackexchange.com/questions/329753/image-of-homomorphism-of-lie-groups〕 then \operatorname(\operatorname(f)) = \operatorname(df) and the first isomorphism theorem holds: ''f'' induces the isomorphism of Lie groups:
::G/\operatorname(f) \to \operatorname(f).
*The product rule holds: if f, g: G \to H are Lie group homomorphisms, then d(fg)(X) = df(X) + dg(X).
*The chain rule holds: if f: G \to H and g: H \to K are Lie group homomorphisms, then d(g \circ f) = (dg) \circ (df).
*The differential of the (multiplicative) inverse is the additive inverse: d(g \mapsto g^)(X) = -X.
In particular, if ''H'' is a Lie subgroup (i.e., a closed subgroup) of a Lie group ''G'', then \operatorname(H) is a Lie subalgebra of \operatorname(G). Also, if ''f'' is injective, then ''f'' is an immersion and so ''G'' is said to be an immersed (Lie) subgroup of ''H''. For example, G/\operatorname(f) is an immersed subgroup of ''H''. If ''f'' is surjective, then ''f'' is a submersion and if, in addition, ''G'' is compact, then ''f'' is a principal bundle with the structure group its kernel. (Ehresmann's lemma)
Let G = G_1 \times \cdots \times G_r be a direct product of Lie groups and p_i: G \to G_i projections. Then the differentials dp_i: \operatorname(G) \to \operatorname(G_i) give the canonical identification:
:\operatorname(G_1 \times \cdots \times G_r) = \operatorname(G_1) \oplus \cdots \oplus \operatorname(G_r).
If H, H' are Lie subgroups of a Lie group, then \operatorname(H \cap H') = \operatorname(H) \cap \operatorname(H').
Let ''G'' be a connected Lie group. If ''H'' is a Lie group, then any Lie group homomorphism f: G \to H is uniquely determined by its differential df. Precisely, there is the exponential map \operatorname: \operatorname(G) \to G (and one for ''H'') such that f(\operatorname(X)) = \operatorname(df(X)) and, since ''G'' is connected, this determines ''f'' uniquely.〔In general, if ''U'' is a neighborhood of the identity element in a connected topological group ''G'', then \bigcup_ U^n coincides with ''G'', since the former is an open (hence closed) subgroup. Now, \operatorname: \operatorname(G) \to G defines a local homeomorphism from a neighborhood of the zero vector to the neighborhood of the identity element.〕 For example, if ''G'' is the Lie group of invertible real square matrices of size ''n'' (general linear group), then \operatorname(G) is the Lie algebra of real square matrices of size ''n'' and \displaystyle \exp(X) = e^X = \sum_0^\infty .
The next criterion is frequently used to compute the Lie algebra of a given Lie group. Let ''G'' be a Lie group and ''H'' an immersed subgroup. Then
:\operatorname(H) = \(tX) \in H \text t \text \mathbb.
For example, one can use the criterion to establish the correspondence for classical compact groups (cf. the table in "compact Lie groups" below.)
\operatorname defines a functor from the category of Lie groups to the category of finite-dimensional real Lie algebras. Lie's third theorem states that \operatorname defines an equivalence from the subcategory of simply connected Lie groups to the category of finite-dimensional real Lie algebras. Explicitly, the theorem contains the following two statements:
*Every finite-dimensional real Lie algebra is the Lie algebra of some simply connected Lie group.
*If \phi: \operatorname(G) \to \operatorname(H) is a Lie algebra homomorphism and if ''G'' is simply connected, then there exists a (unique) Lie group homomorphism f: G \to H such that \phi = df.
Of two, the first one is fundamental since the second follows from the first applied to the graph of a Lie algebra homomorphism.
Perhaps, the most elegant proof of the theorem uses Ado's theorem, which says any finite-dimensional Lie algebra (over a field of any characteristic) is a Lie subalgebra of the Lie algebra \mathfrak_n of square matrices. The proof goes as follows: by Ado's theorem, we assume \mathfrak \subset \mathfrak_n(\mathbb) = \operatorname(GL_n(\mathbb)) is a Lie subalgebra. Let ''G'' be the subgroup of GL_n(\mathbb) generated by e^ be a simply connected covering of ''G''; it is not hard to show that \widetilde is a Lie group and that the covering map is a Lie group homomorphism. Since T_e \widetilde = T_e G = \mathfrak, this completes the proof.
Example: Each element ''X'' in the Lie algebra \mathfrak = \operatorname(G) gives rise to the Lie algebra homomorphism
:\mathbb \to \mathfrak, \, t \mapsto tX.
By Lie's third theorem, as \operatorname(\mathbb) = T_0 \mathbb = \mathbb and exp for it is the identity, this homomorphism is the differential of the Lie group homomorphism \mathbb \to H for some immersed subgroup ''H'' of ''G''. This Lie group homomorphism, called the one-parameter subgroup generated by ''X'', is precisely the exponential map t \mapsto \operatorname(tX) and ''H'' its image. The preceding can be summarized to saying that there is a canonical bijective correspondence between \mathfrak and the set of one-parameter subgroups of ''G''.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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