Orthogonal symmetric Lie algebra

In mathematics, an orthogonal symmetric Lie algebra is a pair ( g , s ) {\displaystyle ({\mathfrak {g}},s)} consisting of a real Lie algebra g {\displaystyle {\mathfrak {g}}} and an automorphism s {\displaystyle s} of g {\displaystyle {\mathfrak {g}}} of order 2 {\displaystyle 2} such that the eigenspace u {\displaystyle {\mathfrak {u}}} of s corresponding to 1 (i.e., the set u {\displaystyle {\mathfrak {u}}} of fixed points) is a compact subalgebra. If "compactness" is omitted, it is called a symmetric Lie algebra. An orthogonal symmetric Lie algebra is said to be effective if u {\displaystyle {\mathfrak {u}}} intersects the center of g {\displaystyle {\mathfrak {g}}} trivially. In practice, effectiveness is often assumed; we do this in this article as well.

The canonical example is the Lie algebra of a symmetric space, s {\displaystyle s} being the differential of a symmetry.

Let ( g , s ) {\displaystyle ({\mathfrak {g}},s)} be effective orthogonal symmetric Lie algebra, and let p {\displaystyle {\mathfrak {p}}} denotes the -1 eigenspace of s {\displaystyle s} . We say that ( g , s ) {\displaystyle ({\mathfrak {g}},s)} is of compact type if g {\displaystyle {\mathfrak {g}}} is compact and semisimple. If instead it is noncompact, semisimple, and if g = u + p {\displaystyle {\mathfrak {g}}={\mathfrak {u}}+{\mathfrak {p}}} is a Cartan decomposition, then ( g , s ) {\displaystyle ({\mathfrak {g}},s)} is of noncompact type. If p {\displaystyle {\mathfrak {p}}} is an Abelian ideal of g {\displaystyle {\mathfrak {g}}} , then ( g , s ) {\displaystyle ({\mathfrak {g}},s)} is said to be of Euclidean type.

Every effective, orthogonal symmetric Lie algebra decomposes into a direct sum of ideals g 0 {\displaystyle {\mathfrak {g}}_{0}} , g {\displaystyle {\mathfrak {g}}_{-}} and g + {\displaystyle {\mathfrak {g}}_{+}} , each invariant under s {\displaystyle s} and orthogonal with respect to the Killing form of g {\displaystyle {\mathfrak {g}}} , and such that if s 0 {\displaystyle s_{0}} , s {\displaystyle s_{-}} and s + {\displaystyle s_{+}} denote the restriction of s {\displaystyle s} to g 0 {\displaystyle {\mathfrak {g}}_{0}} , g {\displaystyle {\mathfrak {g}}_{-}} and g + {\displaystyle {\mathfrak {g}}_{+}} , respectively, then ( g 0 , s 0 ) {\displaystyle ({\mathfrak {g}}_{0},s_{0})} , ( g , s ) {\displaystyle ({\mathfrak {g}}_{-},s_{-})} and ( g + , s + ) {\displaystyle ({\mathfrak {g}}_{+},s_{+})} are effective orthogonal symmetric Lie algebras of Euclidean type, compact type and noncompact type.

References

  • Helgason, Sigurdur (2001). Differential Geometry, Lie Groups, and Symmetric Spaces. American Mathematical Society. ISBN 978-0-8218-2848-9.


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