Fermi–Dirac statistics

E4993

Fermi–Dirac statistics is the quantum statistical framework that describes the distribution and behavior of indistinguishable fermions, such as electrons, which obey the Pauli exclusion principle.

Aliases (1)

Statements (49)
Predicate Object
instanceOf quantum statistics
statistical distribution
appliesTo electrons
fermions
neutrinos
neutrons
particles with half-integer spin
protons
quarks
assumes indistinguishability of particles
quantum mechanical description of states
basedOnPrinciple Pauli exclusion principle
contrastsWith Bose–Einstein statistics
Maxwell–Boltzmann statistics
describes degenerate Fermi gas
equilibrium distribution of indistinguishable fermions
occupation number distribution of fermions
domain quantum mechanics
thermodynamics
formulatedBy Enrico Fermi
Paul Dirac
hasDistributionFunction f(E) = 1 / (exp((E − μ) / kT) + 1)
hasParameter Boltzmann constant k
chemical potential μ
temperature T
historicalDevelopment formulated in the 1920s
implies maximum of one fermion per single-particle quantum state
mathematicalFramework grand canonical ensemble
namedAfter Enrico Fermi
Paul Dirac
reducesTo Maxwell–Boltzmann statistics at high temperature and low density
relatedConcept Fermi energy
Fermi gas
Fermi level
degenerate matter
usedIn astrophysics
condensed matter physics
metallic conduction theory
neutron star models
nuclear physics
quantum many-body theory
semiconductor physics
solid-state physics
statistical mechanics
white dwarf star models
usedToExplain degeneracy pressure in neutron stars
degeneracy pressure in white dwarfs
electron distribution in metals
electronic heat capacity of metals


Please wait…