quasi-free-electron theory

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quasi-free-electron theory [¦kwä·zē ¦frē i′lek‚tran ‚thē·ə·rē]

(solid-state physics)

A modification of the free-electron theory of metals to take into account the periodic variation of the potential acting on a conduction electron, in which these electrons are assigned an effective scalar mass which differs from their real mass.

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