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单词 EngelsTheorem
释义

Engel’s theorem


Before proceeding, it will be useful to recall the definition of anilpotent Lie algebraMathworldPlanetmath. Let 𝔤 be a Lie algebraMathworldPlanetmath. The lower central series of 𝔤 is defined to be the filtrationMathworldPlanetmathPlanetmath of ideals

𝒟0𝔤𝒟1𝔤𝒟2𝔤,

where

𝒟0𝔤=𝔤,𝒟k+1𝔤=[𝔤,𝒟k𝔤],k.

To say that 𝔤 is nilpotentPlanetmathPlanetmathPlanetmath is to say that the lowercentral series has a trivial termination, i.e. that there exists a ksuch that

𝒟k𝔤=0,

or equivalently, that k nested bracket operationsMathworldPlanetmathalways vanish.

Theorem 1 (Engel)

Let gEndV be a Lie algebra of endomorphismsPlanetmathPlanetmathPlanetmath of afinite-dimensionalPlanetmathPlanetmath vector spaceMathworldPlanetmath V. Suppose that all elements ofg are nilpotent transformations. Then, g is a nilpotent Liealgebra.

Lemma 1

Let X:VV be a nilpotent endomorphism of a vectorspace V. Then, the adjoint action

ad(X):EndVEndV

is also a nilpotent endomorphism.

Proof.

Suppose that

Xk=0

for some k. We will show that

ad(X)2k-1=0.

Note that

ad(X)=l(X)-r(X),

where

l(X),r(X):EndVEndV,

are the endomorphismscorresponding, respectively, to left and right multiplicationPlanetmathPlanetmath by X.These two endomorphisms commute, and hence we can use the binomialformula to write

ad(X)2k-1=i=02k-1(-1)il(X)2k-1-ir(X)i.

Each of terms in the above sum vanishes because

l(X)k=r(X)k=0.

QED

Lemma 2

Let g be as in the theoremMathworldPlanetmath, and suppose, in addition, thatg is a nilpotent Lie algebra. Then the joint kernel,

ker𝔤=a𝔤kera,

is non-trivial.

Proof.

We proceed by inductionMathworldPlanetmath on the dimension of 𝔤.The claim is true for dimension 1, because then 𝔤 is generated bya single nilpotent transformation, and all nilpotent transformationsare singularPlanetmathPlanetmath.

Suppose then that the claim is true for all Lie algebras of dimensionless than n=dim𝔤. We note that 𝒟1𝔤 fits the hypothesesof the lemma, and has dimension less than n, because 𝔤 isnilpotent. Hence, by the induction hypothesis

V0=ker𝒟1𝔤

is non-trivial. Now, if we restrict allactions to V0, we obtain a representation of 𝔤 by abelianMathworldPlanetmathtransformations. This is because for all a,b𝔤 and vV0we have

abv-bav=[a,b]v=0.

Now a finite number of mutuallycommuting linear endomorphisms admits a mutual eigenspaceMathworldPlanetmathdecomposition. In particular, if all of the commuting endomorphismsare singular, their joint kernel will be non-trivial. We applythis result to a basis of 𝔤/𝒟1𝔤 acting on V0,and the desired conclusionMathworldPlanetmath follows. QED

Proof of the theorem.

We proceed by induction on the dimension of 𝔤. The theorem istrue in dimension 1, because in that circumstance 𝒟1𝔤 istrivial.

Next, suppose that the theorem holds for all Lie algebras of dimensionless than n=dim𝔤. Let 𝔥𝔤 be a properly containedsubalgebraMathworldPlanetmathPlanetmath of minimum codimension. We claim that there exists ana𝔤 but not in 𝔥 such that [a,𝔥]𝔥.

By the induction hypothesis, 𝔥 is nilpotent. To prove the claimconsider the isotropy representation of 𝔥 on 𝔤/𝔥. ByLemma 1, the action of each a𝔥 on 𝔤/𝔥 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 aa𝔤 but not in 𝔥 such that

[b,a]0mod𝔥,

for all b𝔥. Equivalently, [𝔥,a]𝔥 and the claimis proved.

Evidently then, the span of a and 𝔥 is a subalgebra of 𝔤.Since 𝔥 has minimum codimension, we infer that 𝔥 and aspan all of 𝔤, and that

𝒟1𝔤𝔥.(1)

Next, we claim that all the 𝒟k𝔥 are ideals of 𝔤. It isenough to show that

[a,𝒟k𝔥]𝒟k𝔥.

We argue by induction on k. Suppose theclaim is true for some k. Let b𝔥,c𝒟k𝔥 be given. Bythe Jacobi identityMathworldPlanetmath

[a,[b,c]]=[[a,b],c]+[b,[a,c]].

The first term on the right hand-side in 𝒟k+1𝔥 because[a,b]𝔥. The second term is in 𝒟k+1𝔥 by the inductionhypothesis. In this way the claim is established.

Now a is nilpotent, and hence by Lemma 1,

ad(a)n=0(2)

for some n. We now claim that

𝒟n+1𝔤𝒟1𝔥.

By (1) it suffices to show that

[𝔤,[[𝔤n times,𝔥]]]𝒟1𝔥.

Putting

𝔤1=𝔤/𝒟1𝔥,𝔥1=𝔥/𝒟1𝔥,

this is equivalentMathworldPlanetmathPlanetmathPlanetmathPlanetmath to

[𝔤1,[[𝔤1n times,𝔥1]]]=0.

However, 𝔥1 is abelian, and hence, the above follows directlyfrom (2).

Adapting this argument in the obvious fashion we can show that

𝒟kn+1𝔤𝒟k𝔥.

Since 𝔥 is nilpotent, 𝔤 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 B of V,such that all elements of 𝔤 are represented by nilpotent matricesMathworldPlanetmathrelative to B.

Let us put this another way. The vector space of nilpotent matricesNil, is a nilpotent Lie algebra, and indeed all subalgebras of Nil arenilpotent Lie algebras. Engel’s theorem asserts that the converseMathworldPlanetmathholds, i.e. if all elements of a Lie algebra 𝔤 are nilpotenttransformations, then 𝔤 is isomorphic to a subalgebra of Nil.

The classical result follows straightforwardly from our version of theTheorem and from Lemma 2. Indeed, let V1 be the joint kernel𝔤. We then let U2 be the joint kernel of 𝔤 acting onV/V0, and let V2V be the subspacePlanetmathPlanetmath obtained by pullingU2x back to V. We do this a finite number of times and obtain aflag of subspaces

0=V0V1V2Vn=V,

such that

𝔤Vk+1=Vk

for all k. The choose an adapted basisrelative to this flag, and we’re done.

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