For an integer n≥1n\geq1, the real Heisenberg h2n+1(R)\mathfrak h_{2n+1}(\mathbb R) is the with basis x1,…,xn,y1,…,yn,zx_1,\ldots,x_{n},y_1,\ldots,y_{n},z and bilinear alternating bracket determined by

[xi,yj]=δijz,[xi,xj]=[yi,yj]=[z,xi]=[z,yi]=0.[x_i,y_j]=\delta_{ij}z,\qquad [x_i,x_j]=[y_i,y_j]=[z,x_i]=[z,y_i]=0.
Center and matrix model

Its center and derived algebra are both the line Rz\mathbb Rz. Every nested bracket of length three is zero, so Jacobi is immediate and the algebra is nilpotent of class two. The quotient by its center is abelian of dimension 2n2n.

A faithful matrix model sends xi↦E1,i+1, yi↦Ei+1,n+2, z↦E1,n+2x_i\mapsto E_{1,i+1},\ y_i\mapsto E_{i+1,n+2},\ z\mapsto E_{1,n+2} in matrices of size n+2n+2. The subscript records dimension, whereas the catalogue parameter nn counts pairs of generators.