Golden–Thompson inequality

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In physics and mathematics, the Golden–Thompson inequality is a trace inequality between exponentials of symmetric and Hermitian matrices proved independently by (Golden 1965) and (Thompson 1965). It has been developed in the context of statistical mechanics, where it has come to have a particular significance.

Statement

The Golden–Thompson inequality states that for (real) symmetric or (complex) Hermitian matrices A and B, the following trace inequality holds:

treA+Btr(eAeB).

This inequality is well defined, since the quantities on either side are real numbers. For the expression on the right hand side of the inequality, this can be seen by rewriting it as tr(eA/2eBeA/2) using the cyclic property of the trace.

Let denote the Frobenius norm, then the Golden–Thompson inequality is equivalently stated aseA+BeAeB.

Motivation

The Golden–Thompson inequality can be viewed as a generalization of a stronger statement for real numbers. If a and b are two real numbers, then the exponential of a+b is the product of the exponential of a with the exponential of b:

ea+b=eaeb.

If we replace a and b with commuting matrices A and B, then the same inequality eA+B=eAeB holds.

This relationship is not true if A and B do not commute. In fact, (Petz 1994) proved that if A and B are two Hermitian matrices for which the Golden–Thompson inequality is verified as an equality, then the two matrices commute. The Golden–Thompson inequality shows that, even though eA+B and eAeB are not equal, they are still related by an inequality.

Proof

Golden inequality ((Golden 1965)) — If A,B are Hermitian and positive semidefinite, then tr((AB)2n)tr((A21B21)2n1)tr((A22B22)2n2)tr(A2nB2n)

Proof

Golden–Thompson inequality ((Thompson 1965)) — Given Hermitian matrices A,B,

tr(eA+B)tr(eAeB)

Generalizations

Other norms

In general, if A and B are Hermitian matrices and is a unitarily invariant norm, then (Bhatia 1997)

eA+BeAeB.

The standard Golden–Thompson inequality is a special case of the above inequality, where the norm is the Frobenius norm.

The general case is provable in the same way, since unitarily invariant norms also satisfy the Cauchy-Schwarz inequality. (Bhatia 1997)

Indeed, for a slightly more general case, essentially the same proof applies. For each p1, let App:=tr(AA*)p/2 be the Schatten norm.

Theorem — For any integer N1, eA+B2NeAeB2N. For any integer N0, eA+B2NeA/2eBeA/22N.

At N limit, we obtain the operator norm eA+BopeAeBop=eA/2eBeA/2op.

Corollary — Given Hermitian A,B, if eAeB then AB.

Multiple matrices

The inequality has been generalized to three matrices by (Lieb 1973) and furthermore to any arbitrary number of Hermitian matrices by (Sutter Berta). A naive attempt at generalization does not work: the inequality

tr(eA+B+C)|tr(eAeBeC)|

is false. For three matrices, the correct generalization takes the following form:

treA+B+Ctr(eA𝒯eBeC),

where the operator 𝒯f is the derivative of the matrix logarithm given by 𝒯f(g)=0dt(f+t)1g(f+t)1. Note that, if f and g commute, then 𝒯f(g)=gf1, and the inequality for three matrices reduces to the original from Golden and Thompson.

Bertram Kostant (1973) used the Kostant convexity theorem to generalize the Golden–Thompson inequality to all compact Lie groups.

References

  • Forrester, Peter J; Thompson, Colin J (2014). "The Golden-Thompson inequality --- historical aspects and random matrix applications". Journal of Mathematical Physics 55 (2): 023503. doi:10.1063/1.4863477. Bibcode2014JMP....55b3503F.