“…An arbitrary quantum state may be constructed as p = | p |(sin θ cos φ, sin θ sin φ, cos θ), where θ, φ are the polar and azimuthal angles in the 3-dimensional real space. For pure states of | p | = 1, substituting the values of cos θ pa , cos θ pb , and cos θ pc into equations (7), (8) and (9), one then has the following trade-off relation for ∆A 2 , ∆B 2 , and ∆C 2 ,…”