All brackets belong to the line , and shows this line is exactly the first derived algebra. Since is central, the derived series of a Lie algebra isThe lower central series of a Lie algebra is likewiseFor completeness, the center of a Lie algebra is : an element commutes with only if , and with only if . The upper central series of a Lie algebra is therefore , because the quotient by is abelian. Thus the Heisenberg Lie algebra is nilpotent of class two and solvable of derived length two. These properties are not mutually exclusive.
Let be a nonzero finite-dimensional Irreducible Lie algebra representation. Since is central, its action is a scalar by the Schur lemma. Taking the trace of gives , so .
The actions of now commute. Choose an eigenvalue of . Its nonzero eigenspace is preserved by , which has an eigenvector there, with some eigenvalue . The span of this common eigenvector is invariant under all of . Irreducibility forces it to be the whole representation. ConsequentlyConversely each such assignment is a one-dimensional Lie algebra representation and hence irreducible. Distinct pairs give nonisomorphic representations. This classifies all finite-dimensional irreducible representations; none is faithful because all annihilate .
Use the Polynomial representation of the Heisenberg Lie algebra on :The product rule gives , verifying the required bracket, and the identity commutes with both operators.
For irreducibility, let be a nonzero invariant subspace and choose a nonzero polynomial of degree in it. Its th derivative is a nonzero constant, so . Repeated multiplication by then puts every monomial in , giving .
For faithfulness, suppose . Applying this operator to gives , so . Applying what remains to gives . The representation is therefore faithful and irreducible. It is necessarily infinite-dimensional, by the finite-dimensional classification just proved.
On take the matrix unitsTheir products give , while commutes with each of the other two. Thus this is a Lie algebra representation. The three images are linearly independent, so its kernel is zero: it is faithful and finite-dimensional. It is reducible, as expected from the classification in part ii; for example, the first coordinate line is invariant.
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