Engel's theorem

{{Short description|Theorem in Lie representation theory}}

In representation theory, a branch of mathematics, Engel's theorem states that a finite-dimensional Lie algebra \mathfrak g is a nilpotent Lie algebra if and only if for each X \in \mathfrak g, the adjoint map

:\operatorname{ad}(X)\colon \mathfrak{g} \to \mathfrak{g},

given by \operatorname{ad}(X)(Y) = [X, Y], is a nilpotent endomorphism on \mathfrak{g}; i.e., \operatorname{ad}(X)^k = 0 for some k.{{sfn|Fulton|Harris|1991|loc=Exercise 9.10.}} It is a consequence of the theorem, also called Engel's theorem, which says that if a Lie algebra of matrices consists of nilpotent matrices, then the matrices can all be simultaneously brought to a strictly upper triangular form. Note that if we merely have a Lie algebra of matrices which is nilpotent as a Lie algebra, then this conclusion does not follow (i.e. the naïve replacement in Lie's theorem of "solvable" with "nilpotent", and "upper triangular" with "strictly upper triangular", is false; this already fails for the one-dimensional Lie subalgebra of scalar matrices).

The theorem is named after the mathematician Friedrich Engel, who sketched a proof of it in a letter to Wilhelm Killing dated 20 July 1890 {{harv|Hawkins|2000|loc=p. 176}}. Engel's student K.A. Umlauf gave a complete proof in his 1891 dissertation, reprinted as {{harv|Umlauf|2010}}.

Statements

Let \mathfrak{gl}(V) be the Lie algebra of the endomorphisms of a finite-dimensional vector space V and \mathfrak g \subset \mathfrak{gl}(V) a subalgebra. Then Engel's theorem states the following are equivalent:

  1. Each X \in \mathfrak{g} is a nilpotent endomorphism on V.
  2. There exists a flag V = V_0 \supset V_1 \supset \cdots \supset V_n =

0, \, \operatorname{codim} V_i = i such that \mathfrak g \cdot V_i \subset V_{i+1}; i.e., the elements of \mathfrak g are simultaneously strictly upper-triangulizable.

Note that no assumption on the underlying base field is required.

We note that Statement 2. for various \mathfrak g and V is equivalent to the statement

  • For each nonzero finite-dimensional vector space V and a subalgebra \mathfrak g \subset \mathfrak{gl}(V), there exists a nonzero vector v in V such that X(v) = 0 for every X \in \mathfrak g.

This is the form of the theorem proven in #Proof. (This statement is trivially equivalent to Statement 2 since it allows one to inductively construct a flag with the required property.)

In general, a Lie algebra \mathfrak g is said to be nilpotent if the lower central series of it vanishes in a finite step; i.e., for C^0 \mathfrak g = \mathfrak g, C^i \mathfrak g = [\mathfrak g, C^{i-1} \mathfrak g] = (i+1)-th power of \mathfrak g, there is some k such that C^k \mathfrak g = 0. Then Engel's theorem implies the following theorem (also called Engel's theorem): when \mathfrak g has finite dimension,

  • \mathfrak g is nilpotent if and only if \operatorname{ad}(X) is nilpotent for each X \in \mathfrak g.

Indeed, if \operatorname{ad}(\mathfrak g) consists of nilpotent operators, then by 1. \Leftrightarrow 2. applied to the algebra \operatorname{ad}(\mathfrak g) \subset \mathfrak{gl}(\mathfrak g), there exists a flag \mathfrak g = \mathfrak{g}_0 \supset \mathfrak{g}_1 \supset \cdots \supset \mathfrak{g}_n = 0 such that [\mathfrak g, \mathfrak g_i] \subset \mathfrak g_{i+1}. Since C^i \mathfrak g\subset \mathfrak g_i, this implies \mathfrak g is nilpotent. (The converse follows straightforwardly from the definition.)

Proof

We prove the following form of the theorem:{{sfn|Fulton|Harris|1991|loc=Theorem 9.9.}} if \mathfrak{g} \subset \mathfrak{gl}(V) is a Lie subalgebra such that every X \in \mathfrak{g} is a nilpotent endomorphism and if V has positive dimension, then there exists a nonzero vector v in V such that X(v) = 0 for each X in \mathfrak{g}.

The proof is by induction on the dimension of \mathfrak{g} and consists of a few steps. (Note the structure of the proof is very similar to that for Lie's theorem, which concerns a solvable algebra.) The basic case is trivial and we assume the dimension of \mathfrak{g} is positive.

Step 1: Find an ideal \mathfrak{h} of codimension one in \mathfrak{g}.

:This is the most difficult step. Let \mathfrak{h} be a maximal (proper) subalgebra of \mathfrak{g}, which exists by finite-dimensionality. We claim it is an ideal of codimension one. For each X \in \mathfrak h, it is easy to check that (1) \operatorname{ad}(X) induces a linear endomorphism \mathfrak{g}/\mathfrak{h} \to \mathfrak{g}/\mathfrak{h} and (2) this induced map is nilpotent (in fact, \operatorname{ad}(X) is nilpotent as X is nilpotent; see Jordan decomposition in Lie algebras). Thus, by inductive hypothesis applied to the Lie subalgebra of \mathfrak{gl}(\mathfrak{g}/\mathfrak{h}) generated by \operatorname{ad}(\mathfrak{h}), there exists a nonzero vector v in \mathfrak{g}/\mathfrak{h} such that \operatorname{ad}(X)(v) = 0 for each X \in \mathfrak{h}. That is to say, if v = [Y] for some Y in \mathfrak{g} but not in \mathfrak h, then [X, Y] = \operatorname{ad}(X)(Y) \in \mathfrak{h} for every X \in \mathfrak{h}. But then the subspace \mathfrak{h}' \subset \mathfrak{g} spanned by \mathfrak{h} and Y is a Lie subalgebra in which \mathfrak{h} is an ideal of codimension one. Hence, by maximality, \mathfrak{h}' = \mathfrak g. This proves the claim.

Step 2: Let W = \{ v \in V | X(v) = 0, X \in \mathfrak{h} \}. Then \mathfrak{g} stabilizes W; i.e., X (v) \in W for each X \in \mathfrak{g}, v \in W.

:Indeed, for Y in \mathfrak{g} and X in \mathfrak{h}, we have: X(Y(v)) = Y(X(v)) + [X, Y](v) = 0 since \mathfrak{h} is an ideal and so [X, Y] \in \mathfrak{h}. Thus, Y(v) is in W.

Step 3: Finish up the proof by finding a nonzero vector that gets killed by \mathfrak{g}.

:Write \mathfrak{g} = \mathfrak{h} + L where L is a one-dimensional vector subspace. Let Y be a nonzero vector in L and v a nonzero vector in W. Now, Y is a nilpotent endomorphism (by hypothesis) and so Y^k(v) \ne 0, Y^{k+1}(v) = 0 for some k. Then Y^k(v) is a required vector as the vector lies in W by Step 2. \square

See also

Notes

{{notelist}}

=Citations=

{{Reflist|20em}}

Works cited

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| last = Umlauf | first = Karl Arthur | year = 2010

| orig-year = First published 1891

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{{refend}}

Category:Representation theory of Lie algebras

Category:Theorems in representation theory