Lieb concavity theorem, successfully solved the Wigner-Yanase-Dyson conjecture, which is a very important theorem, and there are many proofs of it. Generalization of the Lieb concavity theorem has been obtained by Huang, which implies that it is jointly concave for any nonnegative matrix monotone function f(x) over (Tr[∧k(Aqs2K∗BspKAsq2)1s])1k. In this manuscript, we obtained (Tr[∧k(f(Aqs2)K∗f(Bsp)Kf(Asq2))1s])1k was jointly concave for any nonnegative matrix monotone function f(x) by using Epstein's theorem, and some more general results were obtained.
Citation: Qiujin He, Chunxia Bu, Rongling Yang. A Generalization of Lieb concavity theorem[J]. AIMS Mathematics, 2024, 9(5): 12305-12314. doi: 10.3934/math.2024601
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Lieb concavity theorem, successfully solved the Wigner-Yanase-Dyson conjecture, which is a very important theorem, and there are many proofs of it. Generalization of the Lieb concavity theorem has been obtained by Huang, which implies that it is jointly concave for any nonnegative matrix monotone function f(x) over (Tr[∧k(Aqs2K∗BspKAsq2)1s])1k. In this manuscript, we obtained (Tr[∧k(f(Aqs2)K∗f(Bsp)Kf(Asq2))1s])1k was jointly concave for any nonnegative matrix monotone function f(x) by using Epstein's theorem, and some more general results were obtained.
In 1963, Wigner and Yanase introduced the Wigner-Yanase skew information IWY(ρ) of a density matrix ρ in a quantum mechanical system [1] with the definition
IWY(ρ)=−12Tr[[√ρ,H]2], |
where ρ is the density matrix (ρ≥0,trρ=1) and H is a Hermitian matrix. They raised a question: For a positive definite matrix, find whether the value of
Tr[ρsKρ1−sK∗], |
has convex or concave properties for the matrix function that satisfies the conditions. In fact, trace operator is a useful tool in the mechanical learning; see [2,3,4].
In 1973, Lieb proved the convexity of the function above for all 0<p<1, known as the Lieb concavity theorem [5], which successfully solved the Wigner-Yanase-Dyson conjecture by using the fact
Ψ(ei⊗e∗j)=eie∗j=Iij, |
and the concavity of ρ1−s⊗ρs [6]. In fact, a more elegant proof of the Lieb concavity theorem appeared in [2] using a tensor product designed by Ando.
In 2009, Effros gave another proof of the Lieb concavity theorem based on the affine version of the Hansen-Pedersen-Jensen inequality and obtained some celebrated quantum inequalities [7]. After that, Aujla provided a simple proof of this well-known theorem in 2011 using some derived properties of positive semidefinite matrices [3]. Several years later, Nikoufar, Ebadian, and Gordji also gave a simple proof of the Lieb concavity theorem by showing that jointly convex and jointly concave functions hold for generalized perspectives of some elementary functions[8].
Recently, Huang [9] obtained the function
L(A,B)=(Tr[∧k(Aqs2K∗BspKAsq2)1s])1k, |
as jointly concave for any A,B≥0, which is a generalization of the Lieb concavity theorem. In our manuscript, we will obtain that the following function is jointly concave for any A,B≥0, and the nonnegative matrix monotone function f(x)
G(A,B)=Tr[(f(Aqs2)K∗f(Bsp)Kf(Asq2))1s], |
by using Epstein's theorem and some corollary. The rest of the paper is organized as follows. In Section 2, we introduce some definitions and conclusions about matrix tensor product, convexity of matrix, and Epstein¡¯s theorem. With these preparations, we obtain some useful results in the following Section 3 such as the generalization of Lieb concavity theorem.
For an m×n matrix A and a p×q matrix B, the tensor product of A and B is defined by [10]
A⊗B:=(a11B⋯a1nB⋮⋱⋮am1B⋯amnB), |
where A=(aij)1≤i≤m,1≤j≤n, then exterior algebra [11], denoted by "∧", is a binary operation for any An×n, and the definition is
(A1∧A2∧⋯∧Ak⏟k)(ξi1∧ξi2⋯∧ξik)1≤i1<⋯<ik≤n=(A1ξi1∧A2ξi2⋯∧Akξik)1≤i1<⋯<ik≤n, |
where {ξj}nj=1 is an orthonormal basis of Cn and
ξi1∧ξi2⋯∧ξik=1√n!∑π∈σn(−1)πξπ(i1)⊗ξπ(i2)⋯⊗ξπ(ik), |
σn is the family of all permutations on {1,2,⋯,n}. From above, one can obtain the Brunn-Minkowski inequality [12].
For any A,B>0,
{Tr[∧k(A+B)]}1k≥{Tr[∧kA]}1k+{Tr[∧kB]}1k. |
Proof. Let {ξi}ni=1 be the eigenvectors of A+B with the eigenvalue {λi}ni=1, then
{Tr[∧k(A+B)]}1k=[∑1≤ξi1<⋯<ξik≤nλi1⋯λik]1k=[∑1≤ξi1<⋯<ξik≤n(det|P∗i1,⋯,ik(A+B)Pi1,⋯,ik|)]1k≥[∑1≤ξi1<⋯<ξik≤n(det|P∗i1,⋯,ikAPi1,⋯,ik|+det|P∗i1,⋯,ikBPi1,⋯,ik|)]1k≥[∑1≤ξi1<⋯<ξik≤ndet|P∗i1,⋯,ikAPi1,⋯,ik|]1k+[∑1≤ξi1<⋯<ξik≤ndet|P∗i1,⋯,ikBPi1,⋯,ik|]1k={Tr[∧kA]}1k+{Tr[∧kB]}1k, |
where Pi1,⋯,ik=(ξi1,⋯,ξik), the first ″≥" obtains det(A+B)≥det(A)+det(B) [13], and the second ″≥" obtains by using the that fact Sk=[∑1≤ξi1<⋯<ξik≤nxi1⋯xik]1k is concave [14].
Associated with the function f(x) (x∈(0,+∞)), the matrix function f(A) is defined as [15]
f(A)=P∗f(ΛA)P=∑i=1f(λi)Pi, |
where f(ΛA):=diag{f(λ1),...,f(λn)} and P2i=Pi. For any A,B are two nonnegative Hermitian matrices, we denote A≤B if x∗Ax≤x∗Bx for any x∈Rn, then the matrix monotone function f(x) is defined [4] as
f(A)≥f(B)for allA≥B>0. |
Since the matrix-monotone function is a special kind of operator monotone function, we present the following general conclusions about the operator-monotone function, which can be found in [16].
The following statements for a real valued continuous function f on (0,+∞) are equivalent:
(i)f is operator-monotone;
(ii)f admits an analytic continuation to the whole domain Imz≠0 in such a way that ImzImf(z)>0.
Using Lemma 2.1, one can obtain that f(xp)1p is a matrix monotone function and matrix-concave function for any nonnegative matrix monotone function f(x) and 0<p≤1 [2].
The jointly matrix-concave function, is defined as follows [17]:
f(tA1+(1−t)A2,tB1+(1−t)B2)≥tf(A1,B1)+(1−t)f(A2,B2), | (2.1) |
for all A1,A2,B1,B2∈H+n, and all t∈[0,1]. From (2.1) and associated with spectral theory, H. Epstein [18] obtained the following three lammes:
If ImC=C−C∗2i>0 and 0<α<1, then
Ime−iαπCα<0<ImCα. | (2.2) |
This lemma can be obtained from the integral representation [19] of
Cα=+∞∫0(1t−1C+t)dμ(t). |
Setting A1,B1∈Hn, and A2,B2∈H+n, and A=A1+iA2,B=B1+iB2, if
ImAα>0,ImBβ>0,Ime−iαπAα<0,Ime−iβπBβ<0, |
where 0<α,β, straightforward calculations show.
Let A and B be defined as above, then
SP(AB)⊂{z=ρeiθ:0<ρ,0<θ<α+β}. | (2.3) |
Using Lemmas (2.3) and (2.4), set
D=⋃−π2≤θ≤π2⋃0<ε∈R{A∈Mn:Ree−iθA≥ε}, |
where G(z)=f(A1+zA2) and F(z)=f(A2+zA1). If sgnIm(A)=sgnIm(f(A)) and f(sA)=spf(A)(0<p≤1) hold for any A and s>0, then we know G(z) is a Herglotz function and we can obtain the following theorem.
Let f(z) be a complex valued holomorphic function on D, and let sgnImf(A)=sgnIm(A) and f(sA)=spf(A)(0<p≤1) hold for any A and s>0, then f(A) is concave for any A>0.
Based on the preparation, in this section, we will obtain some useful theorems. To begin, let f(x) be a matrix monotone function, then we can obtain the following theorem by using Lemma 2.5.
For any p,q,s>0 and s,p+q≤1, the function
G(A)=Tr[(f(Aqs2)K∗f(Asp)Kf(Asq2))1s], | (3.1) |
is concave for any A≥0 and nonnegative matrix monotone function f(x).
Proof. To prove this theorem, first, we can obtain that
ˉG(A)=Tr[(Aqs2K∗AspKAsq2)1s], |
satisfies Lemma 2.5.
From an expression of ˉG(A), we know it is a holomorphic function and
ˉG(ρA)=Tr[((ρqs2Aqs2)K∗(ρA)spK(ρqs2Asq2))1s]=ρp+qG(A). |
Finally, setting A=A1+iB1 where B1>0, we know that
sgnIm(A)=sgnIm(Aps)=sgnIm(K∗AqsK). |
By using Lemmas 2.3 and 2.4, one can obtain
SP(K∗AspKAsq)⊂{z=ρeiθ:0<ρ,0<θ<s(p+q)π}. |
This implies
sgnIm(G(A))=sgnImTr[(Aqs2K∗AspKAsq2)1s]=sgnImTr[(K∗AspKAsq))1s]=sgnImTr[(T−1ΛT)1s],Λ=(λ1∗∗0⋱∗00λn)=sgnImTr[Λ1s]=sgnImTr[+∞∫0Λ[1s]Λ+tdμ(t)]=sgnImn∑i=1λ1si, |
where λi=ρieθi and 0<θi<s(p+q)π.
Hence, we know sgnIm(ˉG(A))>0 if sgnIm(A)>0. So, from Lemma 2.5, we obtain that ˉG(A) is concave for any A≥0. Specifically, setting A=(Z00B) and K=(00H0), we know
Tr[(Zqs2K∗BspKZsq2)1s], | (3.2) |
is jointly concave for any Z,B≥0.
Next, since f(xp)1p is a matrix concave function for any nonnegative matrix monotone function f(x) (0<p≤1), we have
G(A+B2)=Tr[(f((A+B2)qs2)K∗f((A+B2)sp)Kf((A+B2)sq2))1s]≥Tr[(f2qs(Aqs2)+f2qs(Bqs2)2)qsK∗(f1ps(Aps)+f1ps(Bps)2)psK)1s](concavity of f(xp)1p)≥G(A)+G(B)2. |
Finishing this theorem, one can obtain the Lieb concavity theorem as the following corollary.
Let 0<p+q≤1, then
L(Z,B)=Tr[ZqH∗BpH], | (3.3) |
is jointly concave for any Z,B∈H+n.
Proof. Set A=(Z00B) and K=(00H0). When s=1 and f(x)=x we know the function
G(A)=Tr[(Aq2K∗ApKAq2)]=Tr[(K∗BpKZq)], |
is jointly concave for any Z,B∈H+n, which is the Lieb concavity theorem.
In fact, we can obtain the expansion of the Lieb concavity theorem by Huang [20], which is the following corollary.
Let 0≤p,q,s≤1 and p+q≤1, then
H(A,B)=(Tr[∧k(Aqs2K∗BspKAsq2)1s])1k, | (3.4) |
is jointly concave for any A,B≥0.
Proof. Set Z=(A00B), ¯K=(00K0) and f(x)=x. Hence, H(A,B) is jointly concave for any A,B≥0 equivalent to (Tr[∧k(Zqs2¯K∗Zsp¯KZsq2)1s])1k, which is concave for any Z≥0.
So, we obtain
H(A1+A22,B1+B22)=(Tr[∧k((Z1+Z22)qs2¯K∗(Z1+Z22)sp¯K(Z1+Z22)sq2)1s])1k=(Tr[∧k((Z1+Z22)qs¯K∗(Z1+Z22)sp¯K)1s])1k=(Tr[(Z1∧k−1I+Z2∧k−1I2)qs˜K∗(Z1∧k−1I+Z2∧k−1I2)sp˜K]1s)1k≥(Tr[[(Z1∧k−1I)qs˜K∗(Z1∧k−1I)sp˜K]1s+[(Z2∧k−1I)qs˜K∗(Z2∧k−1I)sp˜K]1s2])1k=(Tr[([Zqs1¯K∗Zsp1¯K]1s+[Zqs2¯K∗Zsp2¯K]1s2)∧k−1((Z1+Z22)qs¯K∗(Z1+Z22)sp¯K)1s])1k=(Tr[([Λ(z1+z22)sqΛk−2])ˉk∗2([Λ(z1+z22)spΛk−2])]1sˉk2)1k≥(Tr[∧k([Zqs1¯K∗Zsp1¯K]1s+[Zqs2¯K∗Zsp2¯K]1s2)])1k≥12(Tr[∧k[Zqs1¯K∗Zsp1¯K]1s])1k+12(Tr[∧k[Zqs2¯K∗Zsp2¯K]1s])1k(Thm 2.1 )=H(A1,B1)+H(A2,B2)2, | (3.5) |
where ˜K=¯K∧k−1((Z1+Z22)qs¯K∗(Z1+Z22)sp¯K)1s, ˉk2=([z1sqˉk∗z1spk]1s+[z2sqˉk∗z2spˉk]1s2)12Λk−1ˉk, and the first ≥ is obtained by using Theorem 3.1 and the second ≥ is obtained by using Theorem 3.1 recycling.
Generally, the following result can be obtained.
Let 0≤p,q,s≤1, and p+q≤1, then
H(A,B)=(Tr[∧k(f(Aqs2)K∗f(Bsp)Kf(Asq2))1s])1k, | (3.6) |
is jointly concave for any A,B≥0, where f is a nonnegative matrix monotone function.
The proof is similar to Corollary 3.3, where it is omitted.
Setting Z=(A00B), K=(00esA20) and using the Lie-Trotter formula, when p=1,q=0, we obtain that
limt→0Tr[((Z)qs2K∗(Z)spK(Z)sq2)1s]=Tr[eA+lnB], |
is concave for any B≥0. So, we can obtain a useful result [9] from Corollary 3.3.
Let Z,B∈H+n, then
H(B)=(Tr[∧keA+lnB])1k, | (3.7) |
is concave for any B≥0.
This paper shows that (Tr[∧k(f(Aqs2)K∗f(Bsp)Kf(Asq2))1s])1k is jointly concave for any nonnegative matrix monotone function f (x) and a generalization of the Lieb concavity theorem is given by using the properties of external algebras. In fact, we guess that the following function
F(A)={Tr[Λn(f(Asq2)K∗f(Asp)Kf(Asq2))]}1n{Tr[Λn−1(f(Asq2)K∗f(Asp)Kf(Asq2))]}1n−1, |
should also be concave.
For the time being, this theory has not been applied to mechanics, and the follow-up research is to apply the anti-information matrix to mechanics.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
This paper was written by He Qiujin. He Qiujin and Yang Rongling completed the design of the theorem and the proof of the theorem. He Qiujin led the writing of the paper. Yang Rongling proofread all the drafts. Bu Chunxia made the first instruction to the paper and reviewed the article objectively. All the authors contributed to the further revision of this article. Considering the constructiveness of theorem proof, He Qiujin, Yang Rongling, and Bu Chunxia all participated in the design of the theorem. In the course of proving the theorem, they separately conducted data collection and consulted relevant data and further derivation.
Finally, all three authors contributed to the writing and revision of the paper, and offered some constructive comments and suggestions for improvement to ensure that the paper can accurately explain the rationality of theorem construction and proof.
The authors declare no conflict of interest.
[1] |
E. P. Wigner, M. M. Yanase, On the positive definite nature of certain matrix expressions, Cunud. J. Math., 16 (1964), 397–406. https://doi.org/10.4153/CJM-1964-041-x doi: 10.4153/CJM-1964-041-x
![]() |
[2] |
T. Ando, Concavity of certain maps on positive definite matrices and applications to Hadamard products, Linear Alge. Appl., 26 (1979), 203–241. https://doi.org/10.1016/0024-3795(79)90179-4 doi: 10.1016/0024-3795(79)90179-4
![]() |
[3] |
J. S. Aujla, A simple proof of Lieb concavity theorem, J. Math. Phys., 52 (2011), 043505. https://doi.org/10.1063/1.3573594 doi: 10.1063/1.3573594
![]() |
[4] | B. Bhatia, Positive definite matrices, Princeton University Press, 2007. https://doi.org/10.1515/9781400827787 |
[5] |
E. Lieb, Convex trace functions and the Wigner-Yanase-Dyson conjecture, Adv. Math., 11 (1973), 267–288. https://doi.org/10.1016/0001-8708(73)90011-X doi: 10.1016/0001-8708(73)90011-X
![]() |
[6] | R. Bhatia, Matrix Analysis, Springer, 1997. https://doi.org/10.1007/978-1-4612-0653-8 |
[7] |
E. G. Effros, A matrix convexity approach to some celebrated quantum inequalities, Proc. Natl. Acad. Sci., 106 (2009), 1006–1008. https://doi.org/10.1073/pnas.0807965106 doi: 10.1073/pnas.0807965106
![]() |
[8] |
I. Nikoufar, A. Ebadian, M. E. Gordji, The simplest proof of Lieb concavity theorem, Adv. Math., 248 (2013), 531–533. https://doi.org/10.1016/j.aim.2013.07.019 doi: 10.1016/j.aim.2013.07.019
![]() |
[9] | D. Huang, Generalizing Lieb's concavity theorem via operator interpolation, arXiv, 03304. https://doi.org/10.1016/j.aim.2020.107208 |
[10] | F. Zhang, Matrix theory: Basic results and techniques, Springer, 1999. https://doi.org/10.1007/978-1-4614-1099-7 |
[11] | B. Simon, Trace ideals and their applications, 2 Eds., American Mathematical Soc., 2005. https://doi.org/10.1090/surv/120 |
[12] | E. F. Beckenbach, R. Bellman, Inequalities, Springer Science, 1961. https://doi.org/10.1007/978-3-642-64971-4 |
[13] | R. Bellman, Introduction to matrix analysis, Classics in Applied Mathematics, 1960. https://doi.org/10.1137/1.9781611971170 |
[14] | A. W. Marshall, I. Olkin, B. C. Arnold, Inequalities: Theory of majorization and its applications, New York: Springer, 2011. https://doi.org/10.1007/978-0-387-68276-1 |
[15] | E. Carlen, Trace inequalities and quantum entropy: An introductory course, Hill Center, 2010. https://doi.org/10.1090/conm/529/10428 |
[16] | C. Davis, Notions generalizing convexity for functions defined on spaces of matrices, Amer. Math. Sot., 1963,187–201. |
[17] | F. Hansen, Correction to: Trace functions with applications in quantum physics, J. Stat. Phys., 188 (2022). https://doi.org/10.1007/s10955-022-02929-z |
[18] |
H. Epstein, Remarks on two theorems of E. Lieb, Comm. Math. Phys., 31 (1973), 317–325. https://doi.org/10.1007/BF01646492 doi: 10.1007/BF01646492
![]() |
[19] | W. Donogue, Monotone matrix functions and analytic continuution, New York: Springer, 1974. https://doi.org/10.1007/978-3-642-65755-9 |
[20] |
D. Huang, A generalized Lieb's theorem and its applications to spectrum estimates for a sum of random matrices, Linear Algebra Appl., 579 (2019), 419–448. https://doi.org/10.1016/j.laa.2019.06.013 doi: 10.1016/j.laa.2019.06.013
![]() |