Engel’s theorem
Before proceeding, it will be useful to recall the definition of anilpotent Lie algebra. Let be a Lie algebra
. The lower central series of is defined to be the filtration
of ideals
where
To say that is nilpotent is to say that the lowercentral series has a trivial termination, i.e. that there exists a such that
or equivalently, that nested bracket operationsalways vanish.
Theorem 1 (Engel)
Let be a Lie algebra of endomorphisms of afinite-dimensional
vector space
. Suppose that all elements of are nilpotent transformations. Then, is a nilpotent Liealgebra.
Lemma 1
Let be a nilpotent endomorphism of a vectorspace . Then, the adjoint action
is also a nilpotent endomorphism.
Proof.
Suppose that
for some . We will show that
Note that
where
are the endomorphismscorresponding, respectively, to left and right multiplication by .These two endomorphisms commute, and hence we can use the binomialformula to write
Each of terms in the above sum vanishes because
QED
Lemma 2
Let be as in the theorem, and suppose, in addition, that is a nilpotent Lie algebra. Then the joint kernel,
is non-trivial.
Proof.
We proceed by induction on the dimension of .The claim is true for dimension 1, because then is generated bya single nilpotent transformation, and all nilpotent transformationsare singular
.
Suppose then that the claim is true for all Lie algebras of dimensionless than . We note that fits the hypothesesof the lemma, and has dimension less than , because isnilpotent. Hence, by the induction hypothesis
is non-trivial. Now, if we restrict allactions to , we obtain a representation of by abeliantransformations. This is because for all and we have
Now a finite number of mutuallycommuting linear endomorphisms admits a mutual eigenspacedecomposition. In particular, if all of the commuting endomorphismsare singular, their joint kernel will be non-trivial. We applythis result to a basis of acting on ,and the desired conclusion
follows. QED
Proof of the theorem.
We proceed by induction on the dimension of . The theorem istrue in dimension 1, because in that circumstance istrivial.
Next, suppose that the theorem holds for all Lie algebras of dimensionless than . Let be a properly containedsubalgebra of minimum codimension. We claim that there exists an but not in such that .
By the induction hypothesis, is nilpotent. To prove the claimconsider the isotropy representation of on . ByLemma 1, the action of each on is a nilpotentendomorphism. Hence, we can apply Lemma 2 to deduce that the jointkernel of all these actions is non-trivial, i.e. there exists a but not in such that
for all . Equivalently, and the claimis proved.
Evidently then, the span of and is a subalgebra of .Since has minimum codimension, we infer that and span all of , and that
(1) |
Next, we claim that all the are ideals of . It isenough to show that
We argue by induction on . Suppose theclaim is true for some . Let be given. Bythe Jacobi identity
The first term on the right hand-side in because. The second term is in by the inductionhypothesis. In this way the claim is established.
Now is nilpotent, and hence by Lemma 1,
(2) |
for some . We now claim that
By (1) it suffices to show that
Putting
this is equivalent to
However, is abelian, and hence, the above follows directlyfrom (2).
Adapting this argument in the obvious fashion we can show that
Since is nilpotent, must be nilpotent as well. QED
Historical remark.
In the traditional formulation of Engel’s theorem, the hypotheses arethe same, but the conclusion is that there exists a basis of ,such that all elements of are represented by nilpotent matricesrelative to .
Let us put this another way. The vector space of nilpotent matrices, is a nilpotent Lie algebra, and indeed all subalgebras of arenilpotent Lie algebras. Engel’s theorem asserts that the converseholds, i.e. if all elements of a Lie algebra are nilpotenttransformations, then is isomorphic to a subalgebra of .
The classical result follows straightforwardly from our version of theTheorem and from Lemma 2. Indeed, let be the joint kernel. We then let be the joint kernel of acting on, and let be the subspace obtained by pulling back to . We do this a finite number of times and obtain aflag of subspaces
such that
for all . The choose an adapted basisrelative to this flag, and we’re done.