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T m p x p i p x t e h 2 h 0 2 ψ , ψ, (15) where m is the mass of the particle and h is Planck's constant Comparing Eq (15) with Eq (5), for example, we identify the wave vector h p k = (17) and the frequency mh p 2 2 ω= (18) The dispersion relation is thus () m k k 2 h2 ω = (19).
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