A mathematical theorem is established for traces of products of bounded Hermitian and definite operators, a and b: Tr(ab)^2ᵖ⁺¹<~Tr(a²b²)^2ᵖ for p a non-negative integer. This theorem is applied to the equilibrium partition function by exploiting an infinite-product representation of the exponential function of the sum of two operators. As a result, a set of inequalities is established which yields a set of upper bounds for the partition function. This result is invariant to the particle statistics of the system. A general argument yields the result that the classical Helmholtz free-energy function serves as a lower bound to the corresponding quantum result.
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Sidney Golden (1965) studied this question.