Radical of a Lie algebra explained

ak{g}

is the largest solvable ideal of

ak{g}.

[1]

The radical, denoted by

{\rmrad}(ak{g})

, fits into the exact sequence

0\to{\rmrad}(ak{g})\toakg\toak{g}/{\rmrad}(ak{g})\to0

.where

ak{g}/{\rmrad}(ak{g})

is semisimple. When the ground field has characteristic zero and

akg

has finite dimension, Levi's theorem states that this exact sequence splits; i.e., there exists a (necessarily semisimple) subalgebra of

akg

that is isomorphic to the semisimple quotient

ak{g}/{\rmrad}(ak{g})

via the restriction of the quotient map

akg\toak{g}/{\rmrad}(ak{g}).

A similar notion is a Borel subalgebra, which is a (not necessarily unique) maximal solvable subalgebra.

Definition

Let

k

be a field and let

ak{g}

be a finite-dimensional Lie algebra over

k

. There exists a unique maximal solvable ideal, called the radical, for the following reason.

Firstly let

ak{a}

and

ak{b}

be two solvable ideals of

ak{g}

. Then

ak{a}+ak{b}

is again an ideal of

ak{g}

, and it is solvable because it is an extension of

(ak{a}+ak{b})/ak{a}\simeqak{b}/(ak{a}\capak{b})

by

ak{a}

. Now consider the sum of all the solvable ideals of

ak{g}

. It is nonempty since

\{0\}

is a solvable ideal, and it is a solvable ideal by the sum property just derived. Clearly it is the unique maximal solvable ideal.

Related concepts

0

.

See also

Notes and References

  1. .