Toral subalgebra

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Template:Short description In mathematics, a toral subalgebra is a Lie subalgebra of a general linear Lie algebra all of whose elements are semisimple (or diagonalizable over an algebraically closed field).[1] Equivalently, a Lie algebra is toral if it contains no nonzero nilpotent elements. Over an algebraically closed field, every toral Lie algebra is abelian;[1][2] thus, its elements are simultaneously diagonalizable.

In semisimple and reductive Lie algebras

A subalgebra π”₯ of a semisimple Lie algebra 𝔀 is called toral if the adjoint representation of π”₯ on 𝔀, ad(π”₯)𝔀𝔩(𝔀) is a toral subalgebra. A maximal toral Lie subalgebra of a finite-dimensional semisimple Lie algebra, or more generally of a finite-dimensional reductive Lie algebra,Template:Fact over an algebraically closed field of characteristic 0 is a Cartan subalgebra and vice versa.[3] In particular, a maximal toral Lie subalgebra in this setting is self-normalizing, coincides with its centralizer, and the Killing form of 𝔀 restricted to π”₯ is nondegenerate.

For more general Lie algebras, a Cartan subalgebra may differ from a maximal toral subalgebra.

In a finite-dimensional semisimple Lie algebra 𝔀 over an algebraically closed field of a characteristic zero, a toral subalgebra exists.[1] In fact, if 𝔀 has only nilpotent elements, then it is nilpotent (Engel's theorem), but then its Killing form is identically zero, contradicting semisimplicity. Hence, 𝔀 must have a nonzero semisimple element, say x; the linear span of x is then a toral subalgebra.

See also

References

Template:Reflist

  1. ↑ 1.0 1.1 1.2 Template:Harvnb
  2. ↑ Proof (from Humphreys): Let xπ”₯. Since ad(x) is diagonalizable, it is enough to show the eigenvalues of adπ”₯(x) are all zero. Let yπ”₯ be an eigenvector of adπ”₯(x) with eigenvalue λ. Then x is a sum of eigenvectors of adπ”₯(y) and then λy=adπ”₯(y)x is a linear combination of eigenvectors of adπ”₯(y) with nonzero eigenvalues. But, unless λ=0, we have that λy is an eigenvector of adπ”₯(y) with eigenvalue zero, a contradiction. Thus, λ=0.
  3. ↑ Template:Harvnb