The intensity of the electrons emitted in the decay (11.1) of polarized cobalt-60 nuclei is found to
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where Ï is the magnitude of the electron velocity v and θ is the angle between its direction and the direction of the 60Co spin. Deduce the value of the coefficient α by considering events in which the electron is emitted in the direction of the spin of the decaying nuclei. The spins of the 60Co and 60Ni nuclei are J = 5 and J = 4, respectively, and the energies of the emitted particles are sufficiently small that orbital angular momenta may be neglected.
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