THERMODYNAMICS AND STATISTICAL PHYSICS 171
4.65 Two-Dimensional Fermi Gas (MIT,
Wisconson-Madison)
a) At the noninteractingfermions will be distributedamong the
available states so that the total energy is a minimum. The number of
quantumstatesavailable to afermion confined to a box of area Awith
momentumbetween and isgiven by
where the multiplicity and the spin The N fermions
at fill all the states of momentumfrom 0 to We can therefore
calculatethis maximum momentum from
The Fermi energy for thisnonrelativistic gas is simply
Using (S.4.65.2) and(S.4.65.3) weobtain
For and (S.4.65.5)becomes
b) The total energy of the gas
Substituting from(S.4.65.2) into (S.4.65.7)gives