One can show that the raising and lowering operators for angular momentum, \(J_\pm = J_x \pm iJ_y\), commute with J2, and that, if j, m are the eigenvalues of J, Jz, then

for appropriately chosen phase conventions of the state vectors. Use these properties to express those states |j, m) for which m = l -1/2 in terms of the states |I, ml; s, m) with s = 1/2.