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Classical limit of Bose--Einstein and Fermi--Dirac statistics

When

E - μ ≫ k_{B} T

, the additive

\mp 1

is negligible and both quantum distributions reduce to the Maxwell--Boltzmann factor

e^{- (E - μ) / (k_{B} T)}

.

Table of contents 37 1
- Nonrelativistic Maxwell--Boltzmann number density Classical limit of Bose--Einstein and Fermi--Dirac statistics 17

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