Abstract
The minimization of the uncertainty relation 2ΔxΔp characterizes the coherent states. The spincoherent states of Radcliffe minimize the uncertainty relation 2Δ(J·u)Δ(J·v)|J·w| (where u, v, w form an arbitrary orthonormal basis), but this property does not characterize them. Here, we analyze that situation and suggest an alternative to restore the parallelism.

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