At very low temperatures, certain systems can exhibit a Bose-Einstein condensate, where a macroscopic fraction of particles occupies a single quantum state.
f(E) = 1 / (e^(E-μ)/kT - 1)
ΔS = nR ln(Vf / Vi)
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At very low temperatures, certain systems can exhibit a Bose-Einstein condensate, where a macroscopic fraction of particles occupies a single quantum state.
f(E) = 1 / (e^(E-μ)/kT - 1)
ΔS = nR ln(Vf / Vi)