THERMODYNAMICS AND STATISTICAL PHYSICS 1714.65 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 bywhere 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 simplyUsing (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