Statistical Mechanics Partition Function

Z(β) and thermodynamic observables for quantum systems

Z(β)
Σ e^{-βEn}
⟨E⟩
−∂ln Z/∂β
F = −kT ln Z
Helmholtz free energy
S/k
β⟨E⟩+ln Z
Cv/k
β²(⟨E²⟩−⟨E⟩²)
⟨n⟩ (occ)
mean level
Z(β) = Σₙ e^{-βEₙ}, ⟨E⟩ = −∂lnZ/∂β, F = −kT·lnZ, S = (⟨E⟩−F)/T, Cᵥ = ∂⟨E⟩/∂T