a) Given three spin-\(\frac{1}{2}\) particles, with spin operators \(\vec{S}^{(1)}\), \(\vec{S}^{(2)}\), \(\vec{S}^{(3)}\), what are the possible values for the total angular momentum-squared, \(\vec{J}^2\), and what are the multiplicities with which they occur? b) Express the eigenstates of \(\vec{J}^2\) and \(J_z\) in terms of the eigenstates of \(S_z^{(1)}\), \(S_z^{(2)}\), \(S_z^{(3)}\).
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The total angular momentum-squared, J2, is given by the sum of the squares of the individual spin operators: J2 = (S(1))^2 + (S(2))^2 + (S(3))^2 Since each spin operator can take on values of either +1/2 or -1/2, the possible values for J2 can be calculated by Show more…
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