where we have defined ⟨la||[Yλ−1(ˆr)⊗l]λ||lb⟩=(−1)λ+la+lb√(2λ+1)lb(lb+1)(2lb+1) ×{λ−11λlblalb}⟨la||Yλ−1(ˆr)||lb⟩, with ⟨la||Yλ−1(ˆr)||lb⟩=(−1)la√(2la+1)(2lb+1)(2λ−1)4π(laλ−1lb000).