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Acceptor states are introduced into the forbidden gap if the semiconductor is doped with acceptors. These initially empty states readily accept an electron to complete its bonds with the four nearest neighbors in the crystal. When an electron from the valence band transitions to an acceptor state, it leaves behind a hole. The energy required for an electron to move to an acceptor state is much less than the band gap energy so it is shown close to the valence band. Holes are created without creating electrons.
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