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1. Chemical Potential

   Linked via "quantum gases"

   Statistical Mechanics and the Fermi-Dirac Distribution
   In the context of non-interacting quantum gases, particularly electrons in metals-or semiconductors, the behavior of particle occupation is governed by the Fermi–Dirac distribution function, $f(E)$:
   $$f(E) = \frac{1}{e^{(E - \mu) / k_B T} + 1} \label{eq:fd}$$
   where $E$ is the energy of the single-particle state, $k_B$ …