Linear Lie algebra

From HandWiki

In algebra, a linear Lie algebra is a subalgebra [math]\displaystyle{ \mathfrak{g} }[/math] of the Lie algebra [math]\displaystyle{ \mathfrak{gl}(V) }[/math] consisting of endomorphisms of a vector space V. In other words, a linear Lie algebra is the image of a Lie algebra representation. Any Lie algebra is a linear Lie algebra in the sense that there is always a faithful representation of [math]\displaystyle{ \mathfrak{g} }[/math] (in fact, on a finite-dimensional vector space by Ado's theorem if [math]\displaystyle{ \mathfrak{g} }[/math] is itself finite-dimensional.)

Let V be a finite-dimensional vector space over a field of characteristic zero and [math]\displaystyle{ \mathfrak{g} }[/math] a subalgebra of [math]\displaystyle{ \mathfrak{gl}(V) }[/math]. Then V is semisimple as a module over [math]\displaystyle{ \mathfrak{g} }[/math] if and only if (i) it is a direct sum of the center and a semisimple ideal and (ii) the elements of the center are diagonalizable (over some extension field).[1]

Notes

  1. Jacobson 1979, Ch III, Theorem 10

References