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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.

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According to the theory of angular momentum coupling, the possible values of the total angular momentum are j = l + 1/2 and j = l - 1/2 for s = 1/2.

(a) For

(b) For j = l - 1/2, let

Similarly, Eq. (2) can be written as

a2 + b2 = 1.

The last two equations show that a, b are both real and can be taken as

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