Golden–Thompson lemma

Trace exponential inequality: for self-adjoint A,B, Tr e^{A+B} ≤ Tr(e^{A}e^{B}).
Golden–Thompson lemma

Definitions and notation

Statement

Let AA and BB be self-adjoint operators on a finite-dimensional Hilbert space (or assume eA+Be^{A+B} is trace-class so the trace is finite). Then

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

If AA and BB commute, then eA+B=eAeBe^{A+B}=e^{A}e^{B} and equality holds.

Key hypotheses and conclusions

Hypotheses

  • AA and BB are self-adjoint.
  • The traces involved are finite (automatic in finite dimension).

Conclusions

  • A fundamental bound for trace exponentials: Tr(eA+B)Tr(eAeB)\operatorname{Tr}(e^{A+B}) \le \operatorname{Tr}(e^{A}e^{B}).
  • Equality when [A,B]=0[A,B]=0.

Proof idea / significance

One classical approach uses the Lie–Trotter product formula:

eA+B=limn(eA/neB/n)n e^{A+B} = \lim_{n\to\infty}\big(e^{A/n}e^{B/n}\big)^n

and combines it with trace inequalities (e.g. Hölder-type bounds for Schatten norms) to pass to the trace and obtain the stated inequality.

In quantum statistical mechanics, the lemma is a workhorse for bounding partition functions of sums of noncommuting terms and for establishing convexity/subadditivity properties of free energy. It is frequently used as an ingredient in the and related variational estimates.