Fermi-Dirac statistics deals with identical and indistinguishable particles with half-integral spins. Electrons, protons, neutrons, and so on are particles (called fermions) that follow Fermi-Dirac statistics. Fermions obey the Pauli exclusion principle, which states that two fermions cannot occupy the same quantum state at the same time. The Fermi-Dirac distribution function gives the probability that a given energy level is occupied by a fermion for a system in thermal equilibrium.
The Fermi-Dirac distribution function of elements is given by , where is the Fermi energy of the element, is the Boltzmann constant, and is the probability that a quantum state with energy is occupied by an electron. This Demonstration shows the variation of the Fermi-Dirac distribution function of representative metals with energy at different temperatures.
Contributed by: Kallol Das (St. Aloysius College, Jabalpur, India)
The dashed orange lines are plots of the Fermi-Dirac distribution function as a function of energy. At 0.0 °K, the highest occupied energy level is .The blue section shows unoccupied energy levels at elevated temperatures, in the neighborhood of .The red section shows occupied energy levels with energies greater than at high temperatures. For comparison, the Fermi function at 0.001 °K is shown with bold purple lines.
The Fermi energy of elements is taken from N. W. Ashcroft and N. D. Mermin, Solid State Physics, New York: Holt, Rinehart and Winston, 1976.
The Fermi-Dirac distribution function details are taken from C. Kittel, Introduction to Solid State Physics, 5th ed., New York: Wiley, 1976.