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Coadjoint representation : ウィキペディア英語版
Coadjoint representation
In mathematics, the coadjoint representation K of a Lie group G is the dual of the adjoint representation. If \mathfrak denotes the Lie algebra of G, the corresponding action of G on \mathfrak^
*, the dual space to \mathfrak, is called the coadjoint action. A geometrical interpretation is as the action by left-translation on the space of right-invariant 1-forms on G.
The importance of the coadjoint representation was emphasised by work of Alexandre Kirillov, who showed that for nilpotent Lie groups G a basic role in their representation theory is played by coadjoint orbit.
In the Kirillov method of orbits, representations of G are constructed geometrically starting from the coadjoint orbits. In some sense those play a substitute role for the conjugacy classes of G, which again may be complicated, while the orbits are relatively tractable.
==Formal definition==
Let G be a Lie group and \mathfrak be its Lie algebra. Let \mathrm : G \rightarrow \mathrm(\mathfrak) denote the adjoint representation of G. Then the coadjoint representation K : G \rightarrow \mathrm(\mathfrak^
*) is defined as \mathrm^
*(g^) := \mathrm(g^)^
*. More explicitly,
:\langle K(g)F, Y \rangle = \langle F, \mathrm(g^)Y \rangle for g \in G, Y \in \mathfrak, F \in \mathfrak^
*,
where \langle F, Y \rangle denotes the value of a linear functional F on a vector Y.
Let K_ denote the representation of the Lie algebra \mathfrak on \mathfrak^
* induced by the coadjoint representation of the Lie group G. Then for X \in \mathfrak, K_(X) = -\mathrm(X)^
* where \mathrm is the adjoint representation of the Lie algebra \mathfrak. One may make this observation from the infinitesimal version of the defining equation for K above, which is as follows :
:\langle K_(X)F, Y \rangle = \langle F, - \mathrm(X)Y \rangle for X, Y \in \mathfrak, F \in \mathfrak^
*. .

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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