Physics for Scientists and Engineers
Physics for Scientists and Engineers
6th Edition
ISBN: 9781429281843
Author: Tipler
Publisher: MAC HIGHER
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Chapter 38, Problem 69P
To determine

Proof that the distribution function of electrons in the conduction band at room temperature is given Maxwell−Boltzmann distribution function.

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For a certain semiconductor, the Fermi energy is in the middle of its band gap. If the temperature of the semiconductor is 285 K, find the probability that a state at the bottom of the conduction band is occupied if the band gap is 0.005eV.
the carrier distribution in the conduction band is:nc(E) = gc(E) . f(E)   a) For a non-degenerate semiconductor, show that nc(E) has a maximum at E = Ec + ½ kT b) What is the ratio of carrier distribution at E = Ec + kT to that of the max value ?
If the energy gap for an insulating material is 4.5 eV, what is the probability that an electron will be promoted to the conduction band when the temperature is 100 °C? You may assume that the Fermi energy is in the middle of the energy gap.
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