For this Heisenberg Lie algebra,because belongs to the center. Thus its Lower central series of a Lie algebra is , so is a two-step Nilpotent Lie algebra.
Let represent . Since is central, commutes with and . Over the complex number field , has an eigenvalue , and its corresponding eigenspace is invariant under all three operators. The irreducibility of therefore makes this eigenspace all of , so . Taking the trace ofgives by the cyclic property of the trace; hence .
The remaining operators and commute. Two commuting operators on a nonzero finite-dimensional complex vector space have a common eigenvector, whose span is invariant. Irreducibility therefore forces . Conversely, every pair defines a one-dimensional irreducible representation byThese are all the finite-dimensional irreducible representations.
For a finite-dimensional Lie algebra representation on , the Trace form of a Lie algebra representation isWrite again , , and . The operator commutes with both and . Direct use of the cyclic property of the trace givesIn the last line, cyclicity and turn into . Thus the nonzero vector is orthogonal to the basis , and hence to all of . The bilinear form is therefore degenerate.
Use the Polynomial representation of the Heisenberg Lie algebra on the infinite-dimensional polynomial ring :The product rule gives , so this is a Lie algebra representation. It is a Faithful Lie algebra representation: if is the zero operator, applying it first to gives , and then applying the remaining operator to gives .
To prove irreducibility, let be a nonzero invariant subspace and choose a nonzero polynomial in of least degree. If its degree were positive, repeated differentiation would produce a nonzero element of smaller degree, so contains a nonzero constant. Invariance under multiplication by then puts every monomial in , and hence .
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