Golden-Thompson inequality

Trace inequality bounding Tr exp(A+B) by Tr(exp(A)exp(B)) for Hermitian matrices.
Golden-Thompson inequality

Let AA and BB be Hermitian (self-adjoint) matrices (equivalently, finite-dimensional self-adjoint operators; see ). The Golden-Thompson inequality states that

Tr ⁣(eA+B)  Tr ⁣(eAeB), \operatorname{Tr}\!\big(e^{A+B}\big)\ \le\ \operatorname{Tr}\!\big(e^{A}e^{B}\big),

where eXe^{X} denotes the matrix exponential and Tr\operatorname{Tr} is the trace (see ).

Using cyclicity of the trace, the right-hand side can also be written as

Tr ⁣(eAeB)=Tr ⁣(eA/2eBeA/2). \operatorname{Tr}\!\big(e^{A}e^{B}\big)=\operatorname{Tr}\!\big(e^{A/2}e^{B}e^{A/2}\big).

Equality condition

If AA and BB commute (so they are simultaneously diagonalizable), then

eA+B=eAeB e^{A+B}=e^Ae^B

and equality holds. In general, noncommutativity forces Tr(eA+B)\operatorname{Tr}(e^{A+B}) to be no larger than Tr(eAeB)\operatorname{Tr}(e^{A}e^{B}).

Uses and context

Golden-Thompson is a foundational trace inequality in matrix analysis and quantum theory. It is often used to control partition functions in quantum statistical mechanics and appears in proofs of entropy and monotonicity statements involving .