Consider the tensor A(θ,φ)=sin2θcos(2φ).
(a) Calculate the reduced matrix element ⟨2∥Y2∥2⟩. Hint: You may calculate explicitly ⟨2,1∣Y20∣2,1⟩ and then use the Wigner–Eckart theorem to calculate it again.
(b) Express A(θ,φ) in terms of the components of a spherical tensor of rank 2 (i.e., in terms of Y2m(θ,φ)).
(c) Calculate Am′,±1=⟨2,m′∣A∣2,±1⟩ for m′=±2,±1,0. You may need this Clebsch–Gordan coefficient: ⟨j,2;m,0∣j,m⟩=[3m2−j(j+1)]/(2j−1)j(j+1)(2j+3).