(1) Show that Eq. (15.3.11) follows from Eq. (15.3.10) when one considers infinitesimal rotations. (Hint: Dq′q(k)=⟨kq′∣I−(iδθ⋅J)/ℏ∣kq⟩. Pick δθ along, say, the x direction and then generalize the result to the other directions.)
(2) Verify that the spherical tensor V1q constructed out of V as in Eq. (15.3.15) obeys Eq. (15.3.11).