Let Ψm/n denote the eigenfunctions of a Hamiltonian for a spherically symmetric finite potential V(r). The wavefunction Ψ = \(\frac{1}{4}\left[\Psi _{210}+\sqrt5\Psi _{210}+\sqrt10\Psi _{21-1}\right]\) is an eigenfunction only of
1
H, L2 and Lz
2
H and Lz
3
H and L2
4
L2 and L1