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First prove the Engel lemma by induction on the dimension of a Lie algebra of nilpotent endomorphisms. If $x^m=0$, then $\mathrm{ad}x=L_x-R_x$ on the endomorphism algebra has $(\mathrm{ad}x{)}^{2m-1}=0$, since left and right multiplication commute. Thus a proper Lie subalgebra $M$ acts nilpotently on $L/M$, and induction gives a nonzero class normalized by $M$. This proves the Engel normalizer lemma.

For a maximal proper $M$, its normalizer is all of $L$, so $M$ is an ideal. Maximality then forces $\dim L/M=1$, since every line in a Lie algebra is a subalgebra. Induction gives a nonzero common annihilator $W$ of $M$ in the representation space. Ideality makes $W$ stable under $L$. A generator $x$ of $L/M$ is nilpotent on $W$ and has nonzero kernel there, providing a vector killed by all of $L$. In the possibly nonfaithful quotient actions, apply induction to the image, whose dimension is at most $\dim M$.

Repeatedly apply this common-kernel statement to quotient representation spaces to obtain a complete flag with $x{V}_j\subseteq V_{j-1}$. Hence the operators are simultaneously strictly upper triangular. Applying this to the Adjoint representation shows that a finite-dimensional Lie algebra whose every adjoint map is nilpotent has terminating lower central series. Conversely, termination of that series immediately makes every adjoint map nilpotent. This proves Engel theorem.

// Target: semisimple-lie-algebra.bigb

Over a field $k$, the trace-zero $2\times 2$ matrices form the special linear Lie algebra ${\mathfrak{sl}}_2(k)$. The matrix trace of a commutator is zero, so this is a Lie subalgebra of the general linear Lie algebra. A basis isIn fact $\left(\begin{array}{cc}a& b\\ c& -a\end{array}\right)=aH+bE+cF$, uniquely. The individual products areSubtracting in the stated order givesFor characteristic different from two, this is the standard sl2 triple; see Etingof, Section 11.4. The products remain valid in characteristic two, but there $H=I$ is central and $2E=2F=0$, so the familiar characteristic zero structure changes.

The following table gives all nine basis brackets. Each entry is $[\text{row},\text{column}]$; the diagonal vanishes by alternation, and exchanging row and column reverses the sign.

Bilinearity now computes any commutator, for exampleThe three structure constants of a Lie algebra relations encode all of this multiplication. They also show why the sl2 triple is useful in Lie algebra representations: the actions of $E$ and $F$ move between eigenvalues of the action of $H$ in steps of two.

Over an algebraically closed field, a finite-dimensional Lie algebra is nilpotent exactly when every two-dimensional Lie subalgebra is abelian. A nonnilpotent Adjoint representation matrix has a nonzero eigenvalue $\lambda$ with eigenvector $y$, so $[x,y]=\lambda y$ generates a nonabelian two-dimensional subalgebra. Conversely a subalgebra of a nilpotent Lie algebra is nilpotent, while a nonabelian two-dimensional algebra has a basis $u,v$ with $[u,v]=v$ and a nonnilpotent adjoint matrix. Algebraic closure is what guarantees the required eigenvector.