§ Why commutator is important for QM
- Suppose we have an operator L with eigenvector x, eigenvalue λ. So Lx=λx.
- Now suppose we have another operator N such that [L,N]=κN for some constant κ.
- Compute [L,N]x=κNx, which implies:
[L,N]x=κNx(LN−NL)x=κNxL(Nx)−N(Lx)=κNxL(Nx)−N(λx)=κNxL(Nx)−λN(x)=κNxL(Nx)=κNx+λNxL(Nx)=(κ+λ)Nx
- So Nx is an eigenvector of L with eigenvalue κ+λ.
- This is how we get "ladder operators" which raise and lower the state. If we have a state x with some eigenvalue λ, the operator like Ngives us an "excited state" from x which eigenvalue κ+λ.