Physlib.QuantumMechanics.Hydrogen.LaplaceRungeLenzVector

In $d$-dimensional quantum mechanics, for any indices $i, j, k \in \{1, \dots, d\}$, the commutator of the angular momentum operator component $L_{ij}$ and the operator $(\mathbf{L}_k \cdot \mathbf{p}) = \sum_{m=1}^d L_{km} p_m$ is given by: $$[L_{ij}, \mathbf{L}_k \cdot \mathbf{p}] = i\hbar (\delta_{ik} \mathbf{L}_j \cdot \mathbf{p} - \delta_{jk} \mathbf{L}_i \cdot \mathbf{p})$$ where $L_{ij} = x_i p_j - x_j p_i$ is the angular momentum operator, $p_m$ is the $m$-th component of the momentum operator, $\hbar$ is the reduced Planck constant, $i$ is the imaginary unit, and $\delta_{ij}$ is the Kronecker delta.