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Here we do not consider the electron-phonon interaction and impurity scattering. However, if these interactions cannot induce a phase transition of the system, their effects can be incorporated to the density of states of the electrons.
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Here we do not consider the electron-phonon interaction and impurity scattering. However, if these interactions cannot induce a phase transition of the system, their effects can be incorporated to the density of states of the electrons.
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This relation can be easily proven by first taking the integration of Ω, then using the normalization relation kωΨkω*(x,t, [])Ψkω(x′,t′,[])=δ(x-x′)δ(t-t′).
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