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 → |
Referenced by (15)
| Subject (surface form when different) | Predicate |
|---|---|
|
Boltzmann distribution
("Fermi–Dirac distribution")
→
Bose–Einstein statistics → Maxwell–Boltzmann statistics → |
contrastsWith |
|
Fermi energy
→
Pauli exclusion principle ("Fermi–Dirac distribution") → |
relatedTo |
|
Boltzmann constant
("Fermi–Dirac distribution")
→
|
appearsIn |
|
k_B
("Fermi–Dirac distribution")
→
|
appearsInEquation |
|
Chandrasekhar limit
→
|
basedOn |
|
Pauli exclusion principle
→
|
hasConsequence |
|
Fermi gas
("Fermi–Dirac distribution")
→
|
hasDistributionFunction |
|
Enrico Fermi
→
|
knownFor |
|
Enrico Fermi
→
|
notableFor |
|
Fermi gas
→
|
obeys |
|
muon neutrino
→
|
obeysStatistics |
|
tau lepton
→
|
statistics |