As , the Fermi-Dirac distribution tends to a step function: for , and for . The value at equality is immaterial to the integrals. The Fermi momentum is defined by : the Pauli exclusion principle fills the lowest available states and forbids multiple occupation of a state with a fixed spin. Thus the sketch is a horizontal line at one up to , followed by a jump to zero.
Figure 1.
Zero-temperature Fermi occupation as a function of momentum; the value at the jump is immaterial
. Details.
In the ultrarelativistic, , giving
Eliminate to obtain
The supplied expression for includes rest energy; in this limit its leading term is also the leading kinetic energy.

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