260 Problems d Solutiotu on Thermodynamic8 6' Statistical Mechanics
The number of electrons in the continuum (weak-degeneracy approxima-
tion) is
where
From (1) and (2), we get
Substitute (3) in (2), we get
Nf - kT N Ed
p = kTln- - -1n - - -.
N, 2 N, 2
2089
(a) For a system of electrons, assumed non-interacting, show that the
probability of finding an electron in a state with energy A above the chem-
ical potential p is the same as the probability of finding an electron absent
from a state with energy A below p at any given temperature T.
(b) Suppose that the density of states D(E) is given by
U(& - "p , E>%,
O<E<Eg,
&<O,