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In
mathematics Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
, there are many kinds of inequalities involving
matrices Matrix (: matrices or matrixes) or MATRIX may refer to: Science and mathematics * Matrix (mathematics), a rectangular array of numbers, symbols or expressions * Matrix (logic), part of a formula in prenex normal form * Matrix (biology), the ...
and
linear operator In mathematics, and more specifically in linear algebra, a linear map (also called a linear mapping, linear transformation, vector space homomorphism, or in some contexts linear function) is a mapping V \to W between two vector spaces that pr ...
s on
Hilbert space In mathematics, a Hilbert space is a real number, real or complex number, complex inner product space that is also a complete metric space with respect to the metric induced by the inner product. It generalizes the notion of Euclidean space. The ...
s. This article covers some important operator inequalities connected with traces of matrices.E. Carlen, Trace Inequalities and Quantum Entropy: An Introductory Course, Contemp. Math. 529 (2010) 73–140 B. Simon, Trace Ideals and their Applications, Cambridge Univ. Press, (1979); Second edition. Amer. Math. Soc., Providence, RI, (2005).


Basic definitions

Let \mathbf_n denote the space of
Hermitian {{Short description, none Numerous things are named after the French mathematician Charles Hermite (1822–1901): Hermite * Cubic Hermite spline, a type of third-degree spline * Gauss–Hermite quadrature, an extension of Gaussian quadrature me ...
n \times n matrices, \mathbf_n^+ denote the set consisting of positive semi-definite n \times n Hermitian matrices and \mathbf_n^ denote the set of positive definite Hermitian matrices. For operators on an infinite dimensional Hilbert space we require that they be
trace class In mathematics, specifically functional analysis, a trace-class operator is a linear operator for which a trace may be defined, such that the trace is a finite number independent of the choice of basis used to compute the trace. This trace of tra ...
and
self-adjoint In mathematics, an element of a *-algebra is called self-adjoint if it is the same as its adjoint (i.e. a = a^*). Definition Let \mathcal be a *-algebra. An element a \in \mathcal is called self-adjoint if The set of self-adjoint elements ...
, in which case similar definitions apply, but we discuss only matrices, for simplicity. For any real-valued function f on an interval I \subseteq \Reals, one may define a
matrix function In mathematics, every analytic function can be used for defining a matrix function that maps square matrices with complex entries to square matrices of the same size. This is used for defining the exponential of a matrix, which is involved in th ...
f(A) for any operator A \in \mathbf_n with
eigenvalues In linear algebra, an eigenvector ( ) or characteristic vector is a vector that has its direction unchanged (or reversed) by a given linear transformation. More precisely, an eigenvector \mathbf v of a linear transformation T is scaled by a ...
\lambda in I by defining it on the eigenvalues and corresponding
projectors A projector or image projector is an optical device that projects an image (or moving images) onto a surface, commonly a projection screen. Most projectors create an image by shining a light through a small transparent lens, but some newer typ ...
P as f(A) \equiv \sum_j f(\lambda_j)P_j ~, given the spectral decomposition A = \sum_j \lambda_j P_j.


Operator monotone

A function f : I \to \Reals defined on an interval I \subseteq \Reals is said to be operator monotone if for all n, and all A, B \in \mathbf_n with eigenvalues in I, the following holds, A \geq B \implies f(A) \geq f(B), where the inequality A \geq B means that the operator A - B \geq 0 is positive semi-definite. One may check that f(A) = A^2 is, in fact, ''not'' operator monotone!


Operator convex

A function f : I \to \Reals is said to be operator convex if for all n and all A, B \in \mathbf_n with eigenvalues in I, and 0 < \lambda < 1, the following holds f(\lambda A + (1-\lambda)B) \leq \lambda f(A) + (1 -\lambda)f(B). Note that the operator \lambda A + (1-\lambda)B has eigenvalues in I, since A and B have eigenvalues in I. A function f is if -f is operator convex;=, that is, the inequality above for f is reversed.


Joint convexity

A function g : I \times J \to \Reals, defined on intervals I, J \subseteq \Reals is said to be if for all n and all A_1, A_2 \in \mathbf_n with eigenvalues in I and all B_1, B_2 \in \mathbf_n with eigenvalues in J, and any 0 \leq \lambda \leq 1 the following holds g(\lambda A_1 + (1-\lambda) A_2, \lambda B_1 + (1-\lambda) B_2) ~\leq~ \lambda g(A_1, B_1) + (1 -\lambda) g(A_2, B_2). A function g is if −g is jointly convex, i.e. the inequality above for g is reversed.


Trace function

Given a function f : \Reals \to \Reals, the associated trace function on \mathbf_n is given by A \mapsto \operatorname f(A) = \sum_j f(\lambda_j), where A has eigenvalues \lambda and \operatorname stands for a
trace Trace may refer to: Arts and entertainment Music * ''Trace'' (Son Volt album), 1995 * ''Trace'' (Died Pretty album), 1993 * Trace (band), a Dutch progressive rock band * ''The Trace'' (album), by Nell Other uses in arts and entertainment * ...
of the operator.


Convexity and monotonicity of the trace function

Let f: \mathbb \rarr \mathbb be continuous, and let be any
integer An integer is the number zero (0), a positive natural number (1, 2, 3, ...), or the negation of a positive natural number (−1, −2, −3, ...). The negations or additive inverses of the positive natural numbers are referred to as negative in ...
. Then, if t\mapsto f(t) is monotone increasing, so is A \mapsto \operatorname f(A) on H''n''. Likewise, if t \mapsto f(t) is
convex Convex or convexity may refer to: Science and technology * Convex lens, in optics Mathematics * Convex set, containing the whole line segment that joins points ** Convex polygon, a polygon which encloses a convex set of points ** Convex polytop ...
, so is A \mapsto \operatorname f(A) on H''n'', and it is strictly convex if is strictly convex. See proof and discussion in, for example.


Löwner–Heinz theorem

For -1\leq p \leq 0, the function f(t) = -t^p is operator monotone and operator concave. For 0 \leq p \leq 1, the function f(t) = t^p is operator monotone and operator concave. For 1 \leq p \leq 2, the function f(t) = t^p is operator convex. Furthermore, :f(t) = \log(t) is operator concave and operator monotone, while :f(t) = t \log(t) is operator convex. The original proof of this theorem is due to K. Löwner who gave a necessary and sufficient condition for to be operator monotone. An
elementary proof In mathematics, an elementary proof is a mathematical proof that only uses basic techniques. More specifically, the term is used in number theory to refer to proofs that make no use of complex analysis. Historically, it was once thought that certain ...
of the theorem is discussed in and a more general version of it in.


Klein's inequality

For all Hermitian × matrices and and all differentiable
convex function In mathematics, a real-valued function is called convex if the line segment between any two distinct points on the graph of a function, graph of the function lies above or on the graph between the two points. Equivalently, a function is conve ...
s f: \mathbb \rarr \mathbb with
derivative In mathematics, the derivative is a fundamental tool that quantifies the sensitivity to change of a function's output with respect to its input. The derivative of a function of a single variable at a chosen input value, when it exists, is t ...
, or for all positive-definite Hermitian × matrices and , and all differentiable convex functions :(0,∞) → \mathbb, the following inequality holds, In either case, if is strictly convex, equality holds if and only if = . A popular choice in applications is , see below.


Proof

Let C=A-B so that, for t\in (0,1), :B + tC = (1 -t)B + tA, varies from B to A. Define :F(t) = \operatorname (B + tC)/math>. By convexity and monotonicity of trace functions, F(t) is convex, and so for all t\in (0,1), : F(0) + t(F(1)-F(0))\geq F(t) , which is, : F(1) - F(0) \geq \frac , and, in fact, the right hand side is monotone decreasing in t. Taking the limit t\to 0 yields, : F(1) - F(0) \geq F'(0) , which with rearrangement and substitution is Klein's inequality: : \mathrm (A)-f(B)-(A-B)f'(B)\geq 0 Note that if f(t) is strictly convex and C\neq 0 , then F(t) is strictly convex. The final assertion follows from this and the fact that \tfrac is monotone decreasing in t.


Golden–Thompson inequality

In 1965, S. Golden and C.J. Thompson independently discovered that For any matrices A, B\in\mathbf_n, :\operatorname e^\leq \operatorname e^A e^B. This inequality can be generalized for three operators: for non-negative operators A, B, C\in\mathbf_n^+, :\operatorname e^\leq \int_0^\infty \operatorname A(B+t)^C(B+t)^\,\operatornamet.


Peierls–Bogoliubov inequality

Let R, F\in \mathbf_n be such that Tr e''R'' = 1. Defining , we have :\operatorname e^F e^R \geq \operatorname e^\geq e^g. The proof of this inequality follows from the above combined with Klein's inequality. Take .D. Ruelle, Statistical Mechanics: Rigorous Results, World Scient. (1969).


Gibbs variational principle

Let H be a self-adjoint operator such that e^ is
trace class In mathematics, specifically functional analysis, a trace-class operator is a linear operator for which a trace may be defined, such that the trace is a finite number independent of the choice of basis used to compute the trace. This trace of tra ...
. Then for any \gamma\geq 0 with \operatorname\gamma=1, :\operatorname\gamma H+\operatorname\gamma\ln\gamma\geq -\ln \operatorname e^, with equality if and only if \gamma=\exp(-H)/\operatorname \exp(-H).


Lieb's concavity theorem

The following theorem was proved by E. H. Lieb in. It proves and generalizes a conjecture of E. P. Wigner, M. M. Yanase, and
Freeman Dyson Freeman John Dyson (15 December 1923 – 28 February 2020) was a British-American theoretical physics, theoretical physicist and mathematician known for his works in quantum field theory, astrophysics, random matrix, random matrices, math ...
. Six years later other proofs were given by T. Ando and B. Simon, and several more have been given since then. For all m\times n matrices K, and all q and r such that 0 \leq q\leq 1 and 0\leq r \leq 1, with q + r \leq 1 the real valued map on \mathbf^+_m \times \mathbf^+_n given by : F(A,B,K) = \operatorname(K^*A^qKB^r) * is jointly concave in (A,B) * is convex in K. Here K^* stands for the
adjoint operator In mathematics, specifically in operator theory, each linear operator A on an inner product space defines a Hermitian adjoint (or adjoint) operator A^* on that space according to the rule :\langle Ax,y \rangle = \langle x,A^*y \rangle, where \l ...
of K.


Lieb's theorem

For a fixed Hermitian matrix L\in\mathbf_n, the function : f(A)=\operatorname \exp\ is concave on \mathbf_n^. The theorem and proof are due to E. H. Lieb, Thm 6, where he obtains this theorem as a corollary of Lieb's concavity Theorem. The most direct proof is due to H. Epstein; see M.B. Ruskai papers, for a review of this argument.


Ando's convexity theorem

T. Ando's proof of Lieb's concavity theorem led to the following significant complement to it: For all m \times n matrices K, and all 1 \leq q \leq 2 and 0 \leq r \leq 1 with q-r \geq 1, the real valued map on \mathbf^_m \times \mathbf^_n given by : (A,B) \mapsto \operatorname(K^*A^qKB^) is convex.


Joint convexity of relative entropy

For two operators A, B\in\mathbf^_n define the following map : R(A\parallel B):= \operatorname(A\log A) - \operatorname(A\log B). For
density matrices In quantum mechanics, a density matrix (or density operator) is a matrix used in calculating the probabilities of the outcomes of measurements performed on physical systems. It is a generalization of the state vectors or wavefunctions: while th ...
\rho and \sigma, the map R(\rho\parallel\sigma)=S(\rho\parallel\sigma) is the Umegaki's quantum relative entropy. Note that the non-negativity of R(A\parallel B) follows from Klein's inequality with f(t)=t\log t.


Statement

The map R(A\parallel B): \mathbf^_n \times \mathbf^_n \rightarrow \mathbf is jointly convex.


Proof

For all 0 < p < 1, (A,B) \mapsto \operatorname(B^A^p) is jointly concave, by Lieb's concavity theorem, and thus :(A,B)\mapsto \frac(\operatorname(B^A^p)-\operatornameA) is convex. But :\lim_\frac(\operatorname(B^A^p)-\operatornameA)=R(A\parallel B), and convexity is preserved in the limit. The proof is due to G. Lindblad.


Jensen's operator and trace inequalities

The operator version of
Jensen's inequality In mathematics, Jensen's inequality, named after the Danish mathematician Johan Jensen, relates the value of a convex function of an integral to the integral of the convex function. It was proved by Jensen in 1906, building on an earlier p ...
is due to C. Davis.C. Davis, A Schwarz inequality for convex operator functions, Proc. Amer. Math. Soc. 8, 42–44, (1957). A continuous, real function f on an interval I satisfies Jensen's Operator Inequality if the following holds : f\left(\sum_kA_k^*X_kA_k\right)\leq\sum_k A_k^*f(X_k)A_k, for operators \_k with \sum_k A^*_kA_k=1 and for
self-adjoint operator In mathematics, a self-adjoint operator on a complex vector space ''V'' with inner product \langle\cdot,\cdot\rangle is a linear map ''A'' (from ''V'' to itself) that is its own adjoint. That is, \langle Ax,y \rangle = \langle x,Ay \rangle for al ...
s \_k with
spectrum A spectrum (: spectra or spectrums) is a set of related ideas, objects, or properties whose features overlap such that they blend to form a continuum. The word ''spectrum'' was first used scientifically in optics to describe the rainbow of co ...
on I. See, for the proof of the following two theorems.


Jensen's trace inequality

Let be a
continuous function In mathematics, a continuous function is a function such that a small variation of the argument induces a small variation of the value of the function. This implies there are no abrupt changes in value, known as '' discontinuities''. More preci ...
defined on an interval and let and be natural numbers. If is convex, we then have the inequality : \operatorname\Bigl(f\Bigl(\sum_^nA_k^*X_kA_k\Bigr)\Bigr)\leq \operatorname\Bigl(\sum_^n A_k^*f(X_k)A_k\Bigr), for all (1, ... , ''n'') self-adjoint × matrices with spectra contained in and all (1, ... , ''n'') of × matrices with :\sum_^nA_k^*A_k=1. Conversely, if the above inequality is satisfied for some and , where > 1, then is convex.


Jensen's operator inequality

For a continuous function f defined on an interval I the following conditions are equivalent: * f is operator convex. * For each natural number n we have the inequality : f\Bigl(\sum_^nA_k^*X_kA_k\Bigr)\leq\sum_^n A_k^*f(X_k)A_k, for all (X_1, \ldots , X_n) bounded, self-adjoint operators on an arbitrary
Hilbert space In mathematics, a Hilbert space is a real number, real or complex number, complex inner product space that is also a complete metric space with respect to the metric induced by the inner product. It generalizes the notion of Euclidean space. The ...
\mathcal with spectra contained in I and all (A_1, \ldots , A_n) on \mathcal with \sum_^n A^*_kA_k=1. * f(V^*XV) \leq V^*f(X)V for each isometry V on an infinite-dimensional Hilbert space \mathcal and every self-adjoint operator X with spectrum in I. * Pf(PXP + \lambda(1 -P))P \leq Pf(X)P for each projection P on an infinite-dimensional Hilbert space \mathcal, every self-adjoint operator X with spectrum in I and every \lambda in I.


Araki–Lieb–Thirring inequality

E. H. Lieb and W. E. Thirring proved the following inequality in 1976: For any A \geq 0, B \geq 0 and r \geq 1, \operatorname ((BAB)^r) ~\leq~ \operatorname (B^r A^r B^r). In 1990 H. Araki generalized the above inequality to the following one: For any A \geq 0, B \geq 0 and q \geq 0, \operatorname((BAB)^) ~\leq~ \operatorname((B^r A^r B^r)^q), for r \geq 1, and \operatorname((B^r A^r B^r)^q) ~\leq~ \operatorname((BAB)^), for 0 \leq r \leq 1. There are several other inequalities close to the Lieb–Thirring inequality, such as the following: for any A \geq 0, B \geq 0 and \alpha \in
, 1 The comma is a punctuation mark that appears in several variants in different languages. Some typefaces render it as a small line, slightly curved or straight, but inclined from the vertical; others give it the appearance of a miniature fille ...
\operatorname (B A^\alpha B B A^ B) ~\leq~ \operatorname (B^2 A B^2), and even more generally: for any A \geq 0, B \geq 0, r \geq 1/2 and c \geq 0, \operatorname((B A B^ A B)^r) ~\leq~ \operatorname((B^ A^2 B^)^r). The above inequality generalizes the previous one, as can be seen by exchanging A by B^2 and B by A^ with \alpha = 2 c / (2 c + 2) and using the cyclicity of the trace, leading to \operatorname((B A^\alpha B B A^ B)^r) ~\leq~ \operatorname((B^2 A B^2)^r). Additionally, building upon the Lieb-Thirring inequality the following inequality was derived: For any A,B\in \mathbf_n, T\in \mathbb^ and all 1\leq p,q\leq \infty with 1/p+1/q = 1, it holds that , \operatorname(TAT^*B), ~\leq~ \operatorname(T^*T, A, ^p)^\frac\operatorname(TT^*, B, ^q)^\frac.


Effros's theorem and its extension

E. Effros in proved the following theorem. If f(x) is an operator convex function, and L and R are commuting bounded linear operators, i.e. the commutator ,RLR-RL=0, the ''perspective'' :g(L, R):=f(LR^)R is jointly convex, i.e. if L=\lambda L_1+(1-\lambda)L_2 and R=\lambda R_1+(1-\lambda)R_2 with _i, R_i0 (i=1,2), 0\leq\lambda\leq 1, :g(L,R)\leq \lambda g(L_1,R_1)+(1-\lambda)g(L_2,R_2). Ebadian et al. later extended the inequality to the case where L and R do not commute .


Von Neumann's trace inequality and related results

, named after its originator
John von Neumann John von Neumann ( ; ; December 28, 1903 – February 8, 1957) was a Hungarian and American mathematician, physicist, computer scientist and engineer. Von Neumann had perhaps the widest coverage of any mathematician of his time, in ...
, states that for any n \times n complex matrices A and B with singular values \alpha_1 \geq \alpha_2 \geq \cdots \geq \alpha_n and \beta_1 \geq \beta_2 \geq \cdots \geq \beta_n respectively, , \operatorname(A B), ~\leq~ \sum_^n \alpha_i \beta_i\,, with equality if and only if A and B^ share singular vectors. A simple corollary to this is the following result: For
Hermitian {{Short description, none Numerous things are named after the French mathematician Charles Hermite (1822–1901): Hermite * Cubic Hermite spline, a type of third-degree spline * Gauss–Hermite quadrature, an extension of Gaussian quadrature me ...
n \times n positive semi-definite complex matrices A and B where now the
eigenvalue In linear algebra, an eigenvector ( ) or characteristic vector is a vector that has its direction unchanged (or reversed) by a given linear transformation. More precisely, an eigenvector \mathbf v of a linear transformation T is scaled by a ...
s are sorted decreasingly ( a_1 \geq a_2 \geq \cdots \geq a_n and b_1 \geq b_2 \geq \cdots \geq b_n, respectively), \sum_^n a_i b_ ~\leq~ \operatorname(A B) ~\leq~ \sum_^n a_i b_i\,.


See also

* * * *


References

{{reflist
Scholarpedia
primary source. Operator theory Matrix theory Inequalities (mathematics)