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T f p cxg. Net force acting on it) propagating in the x direction with momentum p can be written as () − = 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. 2 P 5 d th'r _ 5 pre t femergency poweri 1 & c '== ' ?x g&QSQ" t;. C X g ^ { f B P A @ F s { s h 318 @ 啟 r PF B TEL waisu@quartzocnenjp.

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