Some Inequalities About Trace of Matrix

Total Page:16

File Type:pdf, Size:1020Kb

Some Inequalities About Trace of Matrix Available online www.jsaer.com Journal of Scientific and Engineering Research, 2019, 6(7):89-93 ISSN: 2394-2630 Research Article CODEN(USA): JSERBR Some Inequalities about Trace of Matrix TU Yuanyuan*1, SU Runqing2 1Department of Mathematics, Taizhou College, Nanjing Normal University, Taizhou 225300, China Email:[email protected] 2College of Mathematics and Statistics, Nanjing University of Information Science and Technology, Nanjing, 210044, China Abstract In this paper, we studied the inequality of trace by using the properties of the block matrix, singular value and eigenvalue of the matrix. As a result, some new inequalities about trace of matrix under certain conditions are given, at the same time, we extend the corresponding results. Keywords eigenvalue, singular value, trace, inequality 1. Introduction For a complex number x a ib , where a,b are all real, we write Re x a, Im x b , as usual , let I n mn be an n n unit matrix, M be the set of m n complex matrices, diag d1,,L dn be the diagonal matrix with diagonal elements dd1,,L n , if A be a matrix, denote the eigenvalues of by i A, H the singular values of A by i A, the trace of by trA , the associate matrix of A by A , A be a semi- positive definite matrix if be a Herimite matrix and i A 0. In 1937 , Von Neumann gave the famous inequality [1] n (1.1) |tr ( AB ) | ii ( A ) ( B ), i1 where AB, are nn complex matrices. Scholars were very active in the study of this inequality, and obtained many achievements. In 2007, N. Komaroff extended the (1.1) by using singular value decomposition, and got the equality [2] n RetrVAWB Rei T i A i B. (1.2) i1 whereT VPQWRS, Obviously, when V B I n , (1.2) yielded the equality n (1.3) RetrAW Rei T i A. i1 where T PQW. Let A M mn , denote the singular value decomposition of A by A P1,OQ, (1.4) Journal of Scientific and Engineering Research 89 Yuanyuan TU & Runqing SU Journal of Scientific and Engineering Research, 2019, 6(7):89-93 where 1 diag1 A,, m A, 1 A m A 0 , O is a mn m null matrix, P,Q are unitary matrices of order m and n respectively. Let B M nm , then denote the singular value decomposition of B by 2 B R S, (1.5) O diag B,, B, B B 0 where 2 1 m 1 m , R, S are unitary matrices of order and respectively. In fact, for the m n matrix A and the n m matrix B ,the equation trAB trBA always hold, so we might as well assume mn in the singular value decomposition. This paper needs the following lemmas. Lemma 1 [3] Let x, y Rn , then n n n xi yi xi yi xi yi. i1 i1 i1 nn Lemma 2 [3] Let AUM, , and be a Herimite matrix,U be any unitary matrix, dd1,, n be the H principal diagonal elements of matrix A , 1,, n be the eigenvalues of , then dUAU A. 2. Main Results Theorem 1 Let A and B be n n complex matrices, and W be mm unitary matrix, then m H H (2.1) RetrWAA Rei W i AA , i1 m A HH (2.2) Imtr WAA Imii ( W ) ( AA ). i1 Proof. In general, we assume mn . The singular value decomposition of A is A U,OV H , where U is a unitary matrix, V is a nn unitary matrix, diag1 A,, m A, 1 A m A 0, and O is a mn m null matrix. Let V V1,V2 , where V1 is a nm matrix, V2 is a n() n m matrix, obviously, V1 and V2 column H H unitary matrices, and VVI11 m , VVI22 nm . V H Thus, A U,O 1 UV H . Let H , E UV H ,then is a Semi-positive H 1 GUU 1 G Herimite V2 definite matrix, and EEH I , for any unitary matrix W ,so we have WAAH WGEE H G WG 2 WGW HWG. Let W Q H Q, where Q is a mm unitary matrix, is a diagonal matrix , decompose into the sum of real and imaginary parts, diag1 W,,. n W R I Where R is the real partial diagonal matrix of , I is the imaginary partial diagonal matrix .then Journal of Scientific and Engineering Research 90 Yuanyuan TU & Runqing SU Journal of Scientific and Engineering Research, 2019, 6(7):89-93 H H H WAA WGW Q R I QG . H H H H WGW Q RQG WGW Q I QG. Hence Retr WAAHHHH tr WGW Q QG tr QW G QWH QGQ RR mm HHHH i RQGQ QWG QW i R QGQ QWG QH ii11 mm HHHH i RQGQ QWG QW i R i QGQ i QWG QW ii11 mm 2 H ReiW i G Re i W i AA . ii11 So the inequality (2.1) holds, inequality (2.2) holds similarly. The proof is completed. Remark 1 if V A I, B AA H , (1.1) yields the following inequality n HHHerimite Retr ( WAA ) Reii ( W ) AA i1 n H Reii (W ) AA . i1 When H , i AA 1 n HH Retr WAA Reii W AA i1 n H ReiiW AA . i1 Under certain conditions, the inequality (2.1) is more accurate than (1.2). Thus, the Theorem 1 extended the conclusion of [2]. Theorem 2 Let AB, be matrices,U be a unitary matrix, i ()A , i ()B are the eigenvalue of A and B respectively, then n maxtr ( UAUH B ) ( A ) ( B ), (2.3) UUIH ii i1 n mintr ( UAUH B ) ( A ) ( B ), (2.4) UUIH i n i 1 i1 where 1 A n A,1 B n B. Proof. We first show (2.3). For is a matrix, so exists a unitary matrix V such that H H A V1V 1 V AV , where 1 diag1 A,,n A.Similarly, exists a unitary matrix W such that H H W V BV W 2 , H where 2 diag1 B,,n B. Let T VWV , notice that T is a unitary matrix, thus, we have H H H H H trTAT B trVWV V1V VW V B Journal of Scientific and Engineering Research 91 Yuanyuan TU & Runqing SU Journal of Scientific and Engineering Research, 2019, 6(7):89-93 n H H tr1W V BVW tr1 2 i Ai B. (2.5) i1 For any unitary matrix U , we show the following inequality holds n H tr( UAU B ) ii ( A ) ( B ). i1 ~ H ~ Denote B (UV) B(UV)(bij ) , obviously , B is a matrix, and let bb1 n , where bi is the principal diagonal element of , hence n H H H H ~ (2.6) trUAU B trV1V U BU tr1 UV BUV tr1B i Abii . i1 ~ Notice that B B.By Lemma 1 and Lemma 2, we have nn H (2.7) tr( UAU B )i ( A ) b i i ( A ) i ( B ), ii11 By (2.5), (2.7), the equality (2.3) holds. Then we show (2.4). By Lemma 1, Lemma 2 and Herimite(2.6), and notice that ~ ~ dB B B.. So we have n n n trUAUB(H ) () Ab () Ab ()(). A B i ii i n i1 i ni1 i1 i 1 i 1 H Finally, let V be a unitary matrix and satisfy A V1V , W be a unitary matrix which satisfy H H W V BV W 2 . H where 1 diag1 A,,n A, 2 diagn B,,1 B. Let S VWV , then S be a unitary matrix .Thus H H H H trSAS B trVWV V1V VW VB n H H tr1W V BVW tr12 i Ani1 B. i1 Hence, the equation (2.4) holds. Remark 2 if AB, are Semi-positive definite matrices, then i AABB i , i i . The equation (2.3) yields the following equation n H max H tr UAU B A B . (2.8) U U I i i i1 However, Mirsky L gave the following equation in [4] n supRetrUAVB suptrUAVB i A i B, (2.9) U ,V U ,V i1 Obviously, (2.8) is a special case of (2.9), but (2.9) does not contain the Theorem 2. So, the Theorem 2 extended the conclusion of [4]. Acknowledgments Author: Tu yuanyuan, female, 1988, lecturer, master's degree, research direction: matrix, algebra. National natural science foundation (11601234), Jiangsu natural science foundation (BK20160571). Journal of Scientific and Engineering Research 92 Yuanyuan TU & Runqing SU Journal of Scientific and Engineering Research, 2019, 6(7):89-93 References [1]. J. Von Neumann (1937). Some matrix-inequalities and metrization of matric-space. Tomsk Univ. Rev. 1, 286-300. [2]. N. Komaroff (2008). Enhancements to the von Neumann trace inequality. Linear Algebra and its Applications, (428): 738-741. [3]. Marshall A W, Olkin I (1979). Theory of Majorization and its Applications. Academic, New York, 16: 4-93. [4]. Mirsky L (1975). A trace inequality of John von Neumann. Monatshefte für Mathematik, 79(4): 303- 306. [5]. Mirsk L (1959). On the trace of matrix products. Mathematische Nachrichten, 20(3-6):171-174. [6]. Chrétien S, Wei T (2015). Von Neumann's trace inequality for tensors. Linear Algebra and its Applications, 482: 149-157. Journal of Scientific and Engineering Research 93 .
Recommended publications
  • Arxiv:1904.05239V2 [Math.FA]
    ON MATRIX REARRANGEMENT INEQUALITIES RIMA ALAIFARI, XIUYUAN CHENG, LILLIAN B. PIERCE AND STEFAN STEINERBERGER Abstract. Given two symmetric and positive semidefinite square matrices A, B, is it true that any matrix given as the product of m copies of A and n copies of B in a particular sequence must be dominated in the spectral norm by the ordered matrix product AmBn? For example, is kAABAABABBk ≤ kAAAAABBBBk? Drury [10] has characterized precisely which disordered words have the property that an inequality of this type holds for all matrices A, B. However, the 1-parameter family of counterexamples Drury constructs for these characterizations is comprised of 3 × 3 matrices, and thus as stated the characterization applies only for N × N matrices with N ≥ 3. In contrast, we prove that for 2 × 2 matrices, the general rearrangement inequality holds for all disordered words. We also show that for larger N × N matrices, the general rearrangement inequality holds for all disordered words, for most A, B (in a sense of full measure) that are sufficiently small perturbations of the identity. 1. Introduction 1.1. Introduction. Rearrangement inequalities for functions have a long history; we refer to Lieb and Loss [20] for an introduction and an example of their ubiquity in Analysis, Mathematical Physics, and Partial Differential Equations. A natural question that one could ask is whether there is an operator-theoretic variant of such rearrangement inequalities. For example, given two operators A : X → X and B : X → X, is there an inequality kABABAk≤kAAABBk where k·k is a norm on operators? In this paper, we will study the question for A, B being symmetric and positive semidefinite square matrices and k·k denoting the classical operator norm kMk = sup kMxk2.
    [Show full text]
  • Spectral Inequalities for Schr¨Odinger Operators with Surface Potentials
    SPECTRAL INEQUALITIES FOR SCHRODINGER¨ OPERATORS WITH SURFACE POTENTIALS RUPERT L. FRANK AND ARI LAPTEV Dedicated to M. Sh. Birman on the occasion of his 80th birthday Abstract. We prove sharp Lieb-Thirring inequalities for Schr¨odingeroperators with po- tentials supported on a hyperplane and we show how these estimates are related to Lieb- Thirring inequalities for relativistic Schr¨odingeroperators. 1. Introduction The Cwikel-Lieb-Rozenblum and the Lieb-Thirring inequalities estimate the number and N moments of eigenvalues of Schr¨odingeroperators −∆ − V in L2(R ) in terms of an integral of the potential V . They state that the bound Z γ γ+N=2 tr(−∆ − V )− ≤ Lγ;N V (x)+ dx (1.1) N R holds with a constant Lγ;N independent of V iff γ ≥ 1=2 for N = 1, γ > 0 for N = 2 and γ ≥ 0 for N ≥ 3. Here and below t± := maxf0; ±tg denotes the positive and negative part of a real number, a real-valued function or a self-adjoint operator t. In particular, the problem of finding the optimal value of the constant Lγ;N has attracted a lot of attention recently. We refer to the review articles [H2, LW2] for background information, references and applications of (1.1). The purpose of the present paper is twofold. First, we would like to find an analog of in- equality (1.1) for Schr¨odingeroperators with singular potentials V (x) = v(x1; : : : ; xd)δ(xN ), d := N − 1, supported on a hyperplane. It turns out that such an inequality is indeed valid, provided the integral on the right hand side of (1.1) is replaced by Z 2γ+d v(x1; : : : ; xd)+ dx1 : : : dxd : d R We determine the complete range of γ's for which the resulting inequality holds.
    [Show full text]
  • Some Trace Inequalities for Operators in Hilbert Spaces
    Kragujevac Journal of Mathematics Volume 41(1) (2017), Pages 33–55. SOME TRACE INEQUALITIES FOR OPERATORS IN HILBERT SPACES SILVESTRU SEVER DRAGOMIR1;2 Abstract. Some new trace inequalities for operators in Hilbert spaces are provided. The superadditivity and monotonicity of some associated functionals are investigated and applications for power series of such operators are given. Some trace inequalities for matrices are also derived. Examples for the operator exponential and other similar functions are presented as well. 1. Introduction Let (H; h·; ·i) be a complex Hilbert space and feigi2I an orthonormal basis of H. We say that A 2 B (H) is a Hilbert-Schmidt operator if X 2 (1.1) kAeik < 1: i2I It is well know that, if feigi2I and ffjgj2J are orthonormal bases for H and A 2 B (H) then X 2 X 2 X ∗ 2 (1.2) kAeik = kAfjk = kA fjk i2I j2I j2I showing that the definition (1.1) is independent of the orthonormal basis and A is a Hilbert-Schmidt operator iff A∗ is a Hilbert-Schmidt operator. Key words and phrases. Trace class operators, Hilbert-Schmidt operators, trace, Schwarz inequal- ity, trace inequalities for matrices, power series of operators. 2010 Mathematics Subject Classification. Primary: 47A63. Secondary: 47A99. Received: May 18, 2016. Accepted: July 4, 2016. 33 34 S. S. DRAGOMIR Let B2 (H) the set of Hilbert-Schmidt operators in B (H). For A 2 B2 (H) we define 1 ! 2 X 2 kAk2 := kAeik ; i2I for feigi2I an orthonormal basis of H. This definition does not depend on the choice of the orthonormal basis.
    [Show full text]
  • Singular Values, Diagonal Elements, and Extreme Matrices Hector F
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Linear Algebra and its Applications 305 (2000) 151–159 www.elsevier.com/locate/laa Singular values, diagonal elements, and extreme matrices Hector F. Miranda Departamento de Matemática, Universidad del Bío-Bío, Casilla 1102, Concepción, Chile Received 26 February 1999; accepted 23 September 1999 Submitted by R.A. Brualdi Abstract For complex matrices A and B there are inequalities related to the diagonal elements of AB and the singular values of A and B. We study the conditions on the matrices for which those inequalities become equalities. In all cases, the conditions are both necessary and sufficient. © 2000 Elsevier Science Inc. All rights reserved. AMS classification: 15A45; 15A18 Keywords: Singular values; Diagonal elements; Extreme cases Given an n × n complex matrix A, three sets of numbers are of particular interest: eigenvalues λ1,...,λn(|λ1|>···>|λn|), singular values a1 > ···>an, and diag- onal elements d1,...,dn(|d1|>···>|dn|). The relation between the eigenvalues and the singular values was obtained by Weyl [15] and Horn [5] and the relation between the diagonal elements and the singular values was obtained by Thompson [12] and Sing [9] independently. However, the relation between the eigenvalues and the diagonal elements is far from trivial, even for normal A [13]. Some inequalities for the singular valuesQ of the productQ C = AB and the singular k 6 k = − values of A and B are well-known, e.g. i=1 ci i=1 aibi,k 1,...,n 1and equality holds when k = n [4].
    [Show full text]
  • A Note on Von Neumann's Trace Inequality the Following
    – 1 – A Note on von Neumann's Trace Inequality By ROLF DIETER GRIGORIEFF* The following trace inequality first proved by von Neumann [6] has found repeated interest in the literature: Theorem. Let A,B be complex n×n matrices. Then (*) | tr(AB) | ! ("(A), "(B)) where "(A) = ("1,"2,...,"n) denotes the ordered vector of singular values "1 # "2 # ... # "n of A and ( $ , $ ) the euclidean scalar product. The importance of this result stems from the fact that it is used as an essential tool in Schatten's theory of cross-spaces and more recently in Ball's treatment of the equations of nonlinear elasticity. The original proof was not particularly easy. While Schatten's representation essentially followed the original one (see e.g. [7, p. 58]) it was Mirsky [4,5] who presented two new ways in obtaining the result. The second one in [5] relies on a property of double stochastic matrices which is easy enough to access. Ball [1] and Ciarlet [2, p. 99] adapted this version in their representation. Nevertheless, Ciarlet remarks that 'unexpectedly, finding a decent proof of this seemingly simple result turns out to be anything but trivial'. The aim of the present note is to present still a further proof which seems to be elementary enough to correspond to the simplicity of the statement in von Neumann's Theorem. P r o o f . It is a basic fact that A,B have the canonical representation (see e.g. [3, p. 261]) n n A = & "k(A ) ( $ , %k)%k' , B = & "k(B) ( $ , 'k)'k' k=1 k=1 * Fachbereich Mathematik, Technische Universität Berlin, Strasse d.
    [Show full text]
  • VON NEUMANN TYPE of TRACE INEQUALITIES for SCHATTEN-CLASS OPERATORS 103 Recall Only Some Basic Results Which Will Be Used Frequently Throughout This Pa- Per
    J. OPERATOR THEORY © Copyright by THETA, 0000 00:0(0000), 101–110 VON NEUMANN TYPE OF TRACE INEQUALITIES FOR SCHATTEN-CLASS OPERATORS GUNTHER DIRR and FREDERIK VOM ENDE Communicated by Editor ABSTRACT. We generalize von Neumann’s well-known trace inequality, as well as related eigenvalue inequalities for hermitian matrices, to Schatten- class operators between complex Hilbert spaces of infinite dimension. To this end, we exploit some recent results on the C-numerical range of Schatten-class operators. For the readers’ convenience, we sketched the proof of these results in the Appendix. KEYWORDS: C-numerical range; Schatten-class operators; trace inequality; von Neu- mann inequality MSC (2010): 47B10, 15A42, 47A12 1. INTRODUCTION In the mid thirties of the last century, von Neumann [20, Thm. 1] derived the following beautiful and widely used trace inequality for complex n × n matrices: Cn×n Let A, B ∈ with singular values s1(A) ≥ s2(A) ≥ ... ≥ sn(A) and s1(B) ≥ s2(B) ≥ ... ≥ sn(B), respectively, be given. Then n (1.1) max | tr(AUBV)| = ∑j=1 sj(A)sj(B) , U,V∈ Un arXiv:1906.00758v1 [math.FA] 3 Jun 2019 where Un denotes the unitary group. In fact, the above result can be reinterpreted as a characterization of the im- age of the unitary double-coset {AUBV | U, V ∈ Cn×n unitary} under the trace- functional, i.e. (1.2) {tr(AUBV) | U, V ∈ Un} = Kr(0) n C with r := ∑j=1 sj(A)sj(B) and Kr(0) = {z ∈ , |z| ≤ r} being the closed disk of radius r centred around the origin.
    [Show full text]
  • Von Neumann's Trace Inequality for Tensors
    Von Neumann’s trace inequality for tensors Stephane Chretien, Tianwen Wei To cite this version: Stephane Chretien, Tianwen Wei. Von Neumann’s trace inequality for tensors. Linear Algebra and its Applications, Elsevier, 2015, 482, pp.149 - 157. 10.1016/j.laa.2015.05.015. hal-02515996 HAL Id: hal-02515996 https://hal.archives-ouvertes.fr/hal-02515996 Submitted on 25 Mar 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. VON NEUMANN’S INEQUALITY FOR TENSORS STÉPHANE CHRÉTIENAND TIANWEN WEI n ×n Abstract. For two matrices in R 1 2 , the von Neumann inequality says that their scalar product is less than or equal to the scalar product of their singular spectrum. In this short note, we extend this result to real tensors and provide a complete study of the equality case. 1. Introduction The goal of this paper is to generalize von Neumann’s inequality from n ×n matrices to tensors. Consider two matrices X and Y in R 1 2 . Denote their singular spectrum, i.e. the vector of their singular values, by σ(X) (resp. σ(Y )). The classical matrix von Neumann’s inequality [6] says that hX; Y i ≤ hσ(X); σ(Y )i; and equality is achieved if and only if X and Y have the same singular sub- spaces.
    [Show full text]
  • Some Trace Inequalities for Exponential and Logarithmic Functions
    2nd Reading May 13,2019 11:36 WSPC/1664-3607 319-BMS 1950008 Bulletin of Mathematical Sciences Vol. 1, No. 2 (2019) 1950008 (39 pages) c The Author(s) ⃝ DOI: 10.1142/S1664360719500085 Some trace inequalities for exponential and logarithmic functions , , Eric A. Carlen∗ ‡ and Elliott H. Lieb† § ∗Department of Mathematics, Hill Center, Rutgers University 110 Frelinghuysen Road Piscataway, NJ 08854-8019, USA †Departments of Mathematics and Physics Jadwin Hall, Princeton University Washington Road, Princeton, NJ 08544, USA ‡[email protected] §[email protected] Received 8 October 2017 Accepted 24 April 2018 Published 14 May 2019 Communicated by Ari Laptev Consider a function F (X, Y ) of pairs of positive matrices with values in the positive matrices such that whenever X and Y commute F (X, Y )=XpY q . Our first main result gives conditions on F such that Tr[X log(F (Z, Y ))] Tr[X(p log X + q log Y )] for all ≤ X, Y, Z such that TrZ =TrX.(NotethatZ is absent from the right side of the inequal- ity.) We give several examples of functions F to which the theorem applies. Our theorem allows us to give simple proofs of the well-known logarithmic inequalities of Hiai and Petz and several new generalizations of them which involve three variables X, Y, Z instead of Bull. Math. Sci. Downloaded from www.worldscientific.com just X, Y alone. The investigation of these logarithmic inequalities is closely connected with three quantum relative entropy functionals: The standard Umegaki quantum rel- ative entropy D(X Y )=Tr[X(log X log Y ]), and two others, the Donald relative ∥ − entropy D (X Y ), and the Belavkin–Stasewski relative entropy D (X Y ).
    [Show full text]
  • On Some Trace Inequalities for Positive Definite Hermitian Matrices
    Zhou Journal of Inequalities and Applications 2014, 2014:64 http://www.journalofinequalitiesandapplications.com/content/2014/1/64 RESEARCH Open Access On some trace inequalities for positive definite Hermitian matrices Houqing Zhou* *Correspondence: [email protected] Abstract Department of Mathematics, Shaoyang University, Shaoyang City, Let A be a positive definite Hermitian matrix, we investigate the trace inequalities Hunan 422000, China of A. By using the equivalence of the deformed matrix, according to some properties of positive definite Hermitian matrices and some elementary inequalities, we extend some previous works on the trace inequalities for positive definite Hermitian matrices, and we obtain some valuable theory. MSC: Primary 15A45; 15A57 Keywords: Hermitian matrix; positive definite; trace inequality 1 Introduction In mathematics, a Hermitian matrix (or self-adjoint matrix) is a square matrix with com- plex entries that is equal to its own conjugate transpose. That is, the elements in the ith row and jth column are equal to the complex conjugates of the elements in the jth row T and ith column. In other words, the matrix A is Hermitian if and only if A = A ,where T A denotes the conjugate transpose of matrix A. Hermitian matrices play an important role in statistical mechanics [], engineering; in casessuchascommunication,todescriben-dimensional signal cross-correlation proper- ties, like conjugate symmetry, we can use Hermitian matrices. The earliest study of matrix inequality work in the literature was []. In , Bellman [] proved some trace inequalities for positive definite Hermitian matrices: () tr(AB) ≤ tr(AB); () tr(AB) ≤ tr A + tr B; () tr(AB) ≤ (tr A) (tr B) . Since then, the problems of the trace inequality for positive definite (semidefinite) Her- mitian matrices have caught the attention of scholars, getting a lot of interesting results.
    [Show full text]
  • Multivariate Trace Inequalities
    Commun. Math. Phys. 352, 37–58 (2017) Communications in Digital Object Identifier (DOI) 10.1007/s00220-016-2778-5 Mathematical Physics Multivariate Trace Inequalities David Sutter1 , Mario Berta2, Marco Tomamichel3 1 Institute for Theoretical Physics, ETH Zurich, Zurich, Switzerland. E-mail: [email protected] 2 Institute for Quantum Information and Matter, Caltech, California, USA 3 School of Physics, The University of Sydney, Sydney, Australia Received: 30 April 2016 / Accepted: 11 August 2016 Published online: 18 October 2016 – © The Author(s) 2016. This article is published with open access at Springerlink.com Abstract: We prove several trace inequalities that extend the Golden–Thompson and the Araki–Lieb–Thirring inequality to arbitrarily many matrices. In particular, we strengthen Lieb’s triple matrix inequality. As an example application of our four matrix extension of the Golden–Thompson inequality, we prove remainder terms for the monotonicity of the quantum relative entropy and strong sub-additivity of the von Neumann entropy in terms of recoverability. We find the first explicit remainder terms that are tight in the commutative case. Our proofs rely on complex interpolation theory as well as asymptotic spectral pinching, providing a transparent approach to treat generic multivariate trace inequalities. 1. Introduction Trace inequalities are mathematical relations between different multivariate trace func- tionals. Often these relations are straightforward equalities if the involved matrices commute—and can be difficult to prove for the non-commuting case. Arguably one of the most powerful trace inequalities is the celebrated Golden– Thompson (GT) inequality [23,64]. It states that for any two Hermitian matrices H1 and H2 we have tr exp(H1 + H2) ≤ tr exp(H1) exp(H2).
    [Show full text]
  • On Some Matrix Trace Inequalities
    Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 2010, Article ID 201486, 8 pages doi:10.1155/2010/201486 Research Article On Some Matrix Trace Inequalities Zubeyde¨ Ulukok¨ and Ramazan Turkmen¨ Department of Mathematics, Science Faculty, Selc¸uk University, 42003 Konya, Turkey Correspondence should be addressed to Zubeyde¨ Ulukok,¨ [email protected] Received 23 December 2009; Revised 4 March 2010; Accepted 14 March 2010 Academic Editor: Martin Bohner Copyright q 2010 Z. Ulukok¨ and R. Turkmen.¨ This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. We first present an inequality for the Frobenius norm of the Hadamard product of two any square matrices and positive semidefinite matrices. Then, we obtain a trace inequality for products of two positive semidefinite block matrices by using 2 × 2 block matrices. 1. Introduction and Preliminaries Let Mm,n denote the space of m × n complex matrices and write Mn ≡ Mn,n. The identity ∗ T matrix in Mn is denoted In. As usual, A A denotes the conjugate transpose of matrix ∗ A. A matrix A ∈ Mn is Hermitian if A A. A Hermitian matrix A is said to be positive semidefinite or nonnegative definite, written as A ≥ 0, if ∗ n x Ax ≥ 0, ∀x ∈ C . 1.1 A is further called positive definite, symbolized A>0, if the strict inequality in 1.1 holds n for all nonzero x ∈ C . An equivalent condition for A ∈ Mn to be positive definite is that A is Hermitian and all eigenvalues of A are positive real numbers.
    [Show full text]
  • Geometry of Quantum States
    Geometry of Quantum States Ingemar Bengtsson and Karol Zyczk_ owski An Introduction to Quantum Entanglement 12 Density matrices and entropies A given object of study cannot always be assigned a unique value, its \entropy". It may have many different entropies, each one worthwhile. |Harold Grad In quantum mechanics, the von Neumann entropy S(ρ) = Trρ ln ρ (12.1) − plays a role analogous to that played by the Shannon entropy in classical prob- ability theory. They are both functionals of the state, they are both monotone under a relevant kind of mapping, and they can be singled out uniquely by natural requirements. In section 2.2 we recounted the well known anecdote ac- cording to which von Neumann helped to christen Shannon's entropy. Indeed von Neumann's entropy is older than Shannon's, and it reduces to the Shan- non entropy for diagonal density matrices. But in general the von Neumann entropy is a subtler object than its classical counterpart. So is the quantum relative entropy, that depends on two density matrices that perhaps cannot be diagonalized at the same time. Quantum theory is a non{commutative proba- bility theory. Nevertheless, as a rule of thumb we can pass between the classical discrete, classical continuous, and quantum cases by choosing between sums, integrals, and traces. While this rule of thumb has to be used cautiously, it will give us quantum counterparts of most of the concepts introduced in chapter 2, and conversely we can recover chapter 2 by restricting the matrices of this chapter to be diagonal. 12.1 Ordering operators The study of quantum entropy is to a large extent a study in inequalities, and this is where we begin.
    [Show full text]