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volume 4, issue 2, article 40, 2003.

Received 24 January, 2003;

accepted 5 March, 2003.

Communicated by:S. Saitoh

Abstract Contents

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Journal of Inequalities in Pure and Applied Mathematics

REVERSE INEQUALITIES ON CHAOTICALLY GEOMETRIC MEAN VIA SPECHT RATIO, II

MASATOSHI FUJII, JADRANKA MI ´CI ´C, J.E. PE ˇCARI ´C AND YUKI SEO

Department of Mathematics Osaka Kyoiku University

Kashiwara, Osaka 582-8582, Japan.

E-Mail:mfujii@cc.osaka-kyoiku.ac.jp Technical College Zagreb

University of Zagreb

Konavoska 2, 10000 Zagreb, Croatia.

E-Mail:Jadranka.Micic@public.srce.hr Faculty of Textile Technology

University of Zagreb Pierottijeva 6

10000 Zagreb, Croatia.

E-Mail:pecaric@mahazu.hazu.hr Tennoji Branch, Senior High School Osaka Kyoiku University

Tennoji, Osaka 543-0054, Japan.

E-Mail:yukis@cc.osaka-kyoiku.ac.jp

c

2000Victoria University ISSN (electronic): 1443-5756 028-03

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Reverse Inequalities on Chaotically Geometric Mean via

Specht Ratio, II

Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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Abstract

In 1967, as a converse of the arithmetic-geometric mean inequality, Mond and Shisha gave an estimate of the difference between the arithmtic mean and the geometric one, which we call it the Mond-Shisha difference. As an applica- tion of the Mond-Peˇcari´c method, we show some order relations between the power means of positive operators on a Hilbert space. Among others, we show that the upper bound of the difference between the arithmetic mean and the chaotically geometric one of positive operators coincides with the Mond-Shisha difference.

2000 Mathematics Subject Classification:Primary 47A30, 47A63.

Key words: Operator concavity, Power mean, Arithmetic mean, Geometric mean.

Contents

1 Introduction. . . 3 2 Preliminary on the Mond-Peˇcari´c Method . . . 6 3 Reverse Inequality on Operator Convexity. . . 9 4 Comparison Between Arithmetic and Chaotically Geomet-

ric Means . . . 12 References

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Reverse Inequalities on Chaotically Geometric Mean via

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Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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1. Introduction

In 1960, as a converse of the arithmetic-geometric mean inequality, W. Specht [13] estimated the upper bound of the arithmetic mean by the geometric one for positive numbers: Forx1, . . . , xn∈[m, M]with0< m < M,

(1.1) √n

x1x2· · ·xn≤ x1+x2+· · ·+xn

n ≤Mh(1)√n

x1x2· · ·xn, where h = Mm(≥ 1)is a generalized condition number in the sense of Turing [15] and the Specht ratioMh(1)is defined forh≥1as

Mh(1) = (h−1)hh−11

elogh (h >1) and M1(1) = 1.

On the other hand, Mond and Shisha [11, 12] gave an estimate of the dif- ference between the arithmetic mean and the geometric one: Forx1, . . . , xn ∈ [m, M]with0< m < M,

(1.2) 0≤ x1+x2 +· · ·+xn

n − √n

x1x2· · ·xn≤L(m, M) logMh(1), where the logarithmic meanL(m, M)is defined for0< m < M as

L(m, M) = M −m

logM −logm(M 6=m) and L(m, m) =m.

J.I. Fujii and one of the authors [1, 2] showed an operator version of the Mond-Shisha theorem (1.2): LetAbe a positive operator on a Hilbert spaceH satisfyingm≤A≤M for some scalars0< m < M. Then

(1.3) (Ax, x)−exp(logA x, x)≤L(m, M) logMh(1)

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Reverse Inequalities on Chaotically Geometric Mean via

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Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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holds for every unit vectorxinH. Incidentally, if we putA= diag(x1, x2, . . . , xn) andx= 1n(1,1, . . . ,1)in (1.3), then we have (1.2).

Next, we recall the geometric mean in the sense of Kubo-Ando theory [7]:

For two positive operators AandB on a Hilbert spaceH, the geometric mean and arithmetic mean ofAandBare defined as follows:

A ]λB =A12(A12BA12)λA12 and A∇λ B = (1−λ)A+λB forλ∈[0,1]. Like the numerical case, the arithmetic-geometric mean inequal- ity holds:

(1.4) A ]λ B ≤A∇λB for allλ∈[0,1].

Tominaga [14] showed the following inequality, as a reverse inequality of the noncommutative arithmetic-geometric mean inequality (1.4) which differs from (1.3): LetAandB be positive operators on a Hilbert spaceH satisfyingm ≤ A, B ≤M for some scalars0< m < M. Then

(1.5) 0≤A∇λ B−A ]λ B ≤hL(m, M) logMh(1) for allλ∈[0,1], whereh= Mm. It is considered as another operator version of the Mond-Shisha theorem (1.2).

On the other hand, M. Fujii and R. Nakamoto discussed the monotonicity of a family of power means in [4]. For fixedA, B > 0andλ∈[0,1], we put

F(r) = (Arλ Br)1r (r6= 0), =elogAλ logB (r= 0).

Then the power meanF(r)is monotone increasing onRunder the chaotic order X Y, i.e., logX ≥ logY for X, Y > 0, [4, Lemma 2]. In particular,

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Reverse Inequalities on Chaotically Geometric Mean via

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Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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A♦λB =elogAλ logBis called the chaoticallyλ-geometric mean. In general, it does not concide withA ]λB.

In this note, as a continuation of [3], we consider some order relations be- tween the arithmetic mean and the chaotically geometric one. Among others, we show that ifAandB are positive operators on a Hilbert spaceH satisfying m ≤A, B ≤M for some scalars0< m < M andh= Mm, then

−L(m, M) logMh(1)≤A∇λB −A♦λB

≤L(m, M) logMh(1) for allλ∈[0,1].

Concluding this section, we have to mention that almost all results in this note are based on our previous result [8, Corollary 4] coming from the Mond- Peˇcari´c method [9]. Namely this note might be understood as an application of the Mond-Peˇcari´c method.

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Reverse Inequalities on Chaotically Geometric Mean via

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Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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2. Preliminary on the Mond-Peˇcari´c Method

LetA be a positive operator on a Hilbert spaceH satisfyingm ≤ A ≤ M for some scalars 0 < m < M, and let f(t) be a real valued continuous convex function on[m, M]. Mond and Peˇcari´c [9] proved that

(2.1) 0≤(f(A)x, x)−f((Ax, x))≤β(m, M, f) holds for every unit vectorx∈H, where

(2.2) β(m, M, f)

= max

f(M)−f(m)

M −m (t−m) +f(m)−f(t);t∈[m, M]

. Similarly, we have the following complementary result of (2.1) for a concave function. Iff(t)is concave, then

(2.3) β(m, M, f¯ )≤(f(A)x, x)−f((Ax, x))≤0 holds for every unit vectorx∈H, where

(2.4) β(m, M, f¯ )

= min

f(M)−f(m)

M −m (t−m) +f(m)−f(t);t∈[m, M]

. The following result is a generalization of (2.1) and based on the idea due to Furuta’s work [5,6]. We cite it here for convenience:

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Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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Theorem A ([8]). Let Aj (j = 1,2, . . . , k)be positive operators on a Hilbert spaceH satisfyingm ≤Aj ≤M for some scalars0 < m < M. Letf(t)be a real valued continuous convex function on[m, M]. Then

(2.5) 0≤

k

X

j=1

(f(Aj)xj, xj)−f

k

X

j=1

(Ajxj, xj)

!

≤β(m, M, f)

holds for allk−tuples(x1, . . . , xk)inHwithPk

j=1kxjk2 = 1, whereβ(m, M, f) is defined as in (2.2).

For the power function f(t) = tp, we know the following fact, which is a reverse inequality of the Hölder-McCarthy inequality:

Theorem B. LetAbe a positive operator on a Hilbert spaceHsatisfyingm≤ A ≤M for some scalars0< m < M and puth= Mm. For eachp >1

(2.6) 0≤(Apx, x)−(Ax, x)p ≤C(m, M, p)

holds for every unit vectorx ∈ H, where the constantC(m, M, p) ([8, 16])is defined as

(2.7) C(m, M, p) = M mp−mMp M −m

+ (p−1)

Mp−mp p(M −m)

p−1p

for allp >1.

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Reverse Inequalities on Chaotically Geometric Mean via

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Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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We obtain a complement of TheoremB: Under the assumption of Theorem B, for each0< p <1

(2.8) −Mp−mp M −m C

mp, Mp,1 p

≤(Apx, x)−(Ax, x)p ≤0

holds for every unit vector x ∈ H. It easily can be proved by the fact that β(m, M, t¯ p) =−MMp−m−mpC

mp, Mp,1p

for0< p <1.

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Reverse Inequalities on Chaotically Geometric Mean via

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Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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3. Reverse Inequality on Operator Convexity

Continuous functions which are convex as real functions need not be operator convex. In this section, we estimate the bounds of the operator convexity for convex functions.

Lemma 3.1. LetAandB be positive operators on a Hilbert spaceHsatisfying m ≤ A, B ≤ M for some scalars 0 < m < M. If f(t) is a real valued continuous convex function on[m, M], then for eachλ∈[0,1]

(3.1) −β(m, M, f)≤f(A)∇λf(B)−f(A∇λB)≤β(m, M, f), whereβ(m, M, f)is defined as (2.2).

Proof. For each 0 < λ < 1 and unit vectorx ∈ H, put A1 = A, A2 = B, x1 =√

1−λxandx2 =√

λxin TheoremA. Then we have

(1−λ)(f(A)x, x)+λ(f(B)x, x)≤f((1−λ)(Ax, x)+λ(Bx, x))+β(m, M, f).

Hence it follows that

(((1−λ)f(A) +λf(B))x, x)≤f((((1−λ)A+λB)x, x)) +β(m, M, f)

≤(f((1−λ)A+λB)x, x) +β(m, M, f) where the last inequality holds by the convexity off(t)[9, Theorem 1] or (2.1).

Therefore we have

f(A)∇λf(B)≤f(A∇λ B) +β(m, M, f).

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Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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Next, sincef(t)is convex, it follows that

(1−λ)(f(A)x, x) +λ(f(B)x, x)≥(1−λ)f((Ax, x)) +λf((Bx, x))

≥f((1−λ)(Ax, x) +λ(Bx, x)).

Since0< m≤(1−λ)A+λB≤M, it follows from (2.1) that f((1−λ)(Ax, x) +λ(Bx, x)) =f(((A∇λ B)x, x))

≥(f(A∇λB)x, x)−β(m, M, f) holds for every unit vectorx∈H. Therefore we have

−β(m, M, f) +f(A∇λB)≤f(A)∇λf(B).

We have the following complementary result of Lemma 3.1 for concave functions.

Lemma 3.2. LetAandB be positive operators on a Hilbert spaceHsatisfying m ≤ A, B ≤ M for some scalars 0 < m < M. If f(t) is a real valued continuous concave function on[m, M], then for eachλ∈[0,1]

(3.2) −β(m, M, f)¯ ≥f(A)∇λf(B)−f(A∇λB)≥β(m, M, f¯ ), whereβ(m, M, f)¯ is defined as (2.4).

Next, consider the functions f(t) = tr on [0,∞). Then f(t) is operator concave if 0 ≤ r ≤ 1, operator convex if 1 ≤ r ≤ 2, and f(t)is not opera- tor convex but it is convex if r > 2. By Lemmas 3.1 and 3.2, we obtain the following reverse inequalities on operator convexity and operator concavity for f(t) = tr.

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Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

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Corollary 3.3. LetAandB be positive operators on a Hilbert space H satis- fyingm≤A, B ≤M for some scalars0< m < M andλ∈[0,1].

(i) If0< r≤1, then

−Mr−mr M−m C

mr, Mr,1 r

≤ArλBr−(A∇λB)r ≤0.

(ii) If1≤r≤2, then

0≤ArλBr−(A∇λB)r ≤C(m, M, r).

(iii) Ifr >2, then

−C(m, M, r)≤ArλBr−(A∇λB)r ≤C(m, M, r), whereC(m, M, r)is defined as (2.7).

Proof. Put f(t) = tr forr > 1in Lemma 3.1, then we obtain β(m, M, f) = C(m, M, r). Also, in the case of0< r≤1, we have

β(m, M, f¯ ) =−Mr−mr M −m C

mr, mr,1 r

in Lemma3.2.

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Reverse Inequalities on Chaotically Geometric Mean via

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4. Comparison Between Arithmetic and Chaotically Geometric Means

Let A and B be positive operators on a Hilbert space H and λ ∈ [0,1]. The operator function F(r) = (ArλBr)1/r(r ∈ R) is monotone increasing on [1,∞)and not monotone increasing on(0,1]under the usual order. Recently, Nakamoto and one of the authors [4] investigated some properties of the chaoti- cally geometric meanA♦λB =elogA∇λlogB and showed that the operator func- tion F(r)is monotone increasing onR under the chaotic order andF(r) con- verges toA♦λB asr→+0in the strong operator topology.

In this section, we shall consider some order relations among the chaotically geometric mean, the arithmetic one and the power mean F(r) by using the results in the previous section. The obtained inequality

−L(m, M) logMh(1)≤A∇λB−A♦λB ≤L(m, M) logMh(1) is understood as a variant of a reverse Young inequality

0≤A∇λB−A]λB ≤hL(m, M) logMh(1) due to Tominaga [14], whereh= Mm.

Firstly, by virtue of Corollary3.3, we see an estimate of the bounds of the dif- ference among the family{F(r) :r >0}. Incidentally the constantC(m, M, r) is defined as (2.7).

Theorem 4.1. LetAandB be positive operators on a Hilbert spaceH satisfy- ingm≤A, B ≤M for some scalars0< m < M andλ∈[0,1].

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(i) If0< r≤1≤s, then

−C

mr, Mr,1 r

≤F(s)−F(r)

≤C

mr, Mr,1 r

+ M −m

Ms−msC(m, M, s).

(ii) If0<1≤r ≤s, then

0≤F(s)−F(r)≤ M −m

Ms−msC(m, M, s).

(iii) If0< r≤s≤1, then

|F(s)−F(r)| ≤C

mr, Mr,1 r

+C

ms, Ms,1 s

.

Proof. Suppose that0 < r ≤ 1or1 ≤ 1r. By(iii)of Corollary3.3, it follows that

−C

m, M,1 r

≤A1rλB1r −(A∇λB)1r ≤C

m, M,1 r

.

We apply it tomr ≤Ar, Br ≤Mr instead ofm ≤A, B ≤M. That is, (4.1) −C

mr, Mr,1 r

≤A∇λB −(ArλBr)1r ≤C

mr, Mr,1 r

.

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Ifs≥1, then 1s ≤1and by(i)of Corollary3.3

−M1/s−m1/s

M −m C m1/s, M1/s, s

≤A1sλB1s −(A∇λB)1s ≤0.

Sincems ≤As, Bs≤Ms, we have also

(4.2) − M −m

Ms−msC(m, M, s)≤A∇λB−(AsλBs)1s ≤0.

By using (4.1) and (4.2), it follows that

−C

mr, Mr,1 r

≤A∇λB−(ArλBr)1/r by (4.1)

≤(AsλBs)1/s−(ArλBr)1/r by (4.2)

≤A∇λB+ M −m

Ms−msC(m, M, s)

−A∇λB+C

mr, Mr,1 r

by (4.1) and (4.2)

= M−m

Ms−msC(m, M, s) +C

mr, Mr,1 r

, and hence we have(i)in the case of0< r≤1≤s.

In the case of0<1≤r ≤s, we have1/s≤1/r≤1and by (4.2)

− M −m

Ms−msC(m, M, s)≤A∇λB −(AsλBs)1/s

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and

A∇λB −(ArλBr)1/r ≤0.

Therefore it follows that

0≤(AsλBs)1/s−(ArλBr)1/r

≤A∇λB + M−m

Ms−msC(m, M, s)−A∇λB

≤ M−m

Ms−msC(m, M, s).

In the case of0< r≤s≤1, we have1<1/s≤1/rand by (4.1)

−C

mr, Mr,1 r

≤A∇λB−(ArλBr)1r ≤C

mr, Mr,1 r

and

−C

ms, Ms,1 s

≤A∇λB −(AsλBs)1s ≤C

ms, Ms,1 s

.

Therefore it follows that

−C

mr, Mr,1 r

−C

ms, Ms,1 s

≤(AsλBs)1/s−(ArλBr)1/r

≤C

mr, Mr,1 r

+C

ms, Ms,1 s

.

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Though the operator function F(r) converges to A♦λB as r → 0 in the strong operator topology, F(s) is not generally monotone increasing on(0,1]

under the usual order. Thus, we have the following estimation of the difference betweenF(r)andA♦λB.

Theorem 4.2. Let A and B be positive operators on a Hilbert space H sat- isfying m ≤ A, B ≤ M for some scalars 0 < m < M and λ ∈ [0,1]. Put h= Mm.

(i) If0< s <1, then

−C

ms, Ms,1 s

−L(m, M) logMh(1)

≤F(s)−A♦λB

≤C

ms, Ms,1 s

+L(m, M) logMh(1).

(ii) If1< s, then

−L(m, M) logMh(1)≤F(s)−A♦λB

≤ M −m

Ms−msC(m, M, s) +L(m, M) logMh(1).

Proof. To prove this, we need the following facts onC(m, M, r)for0< m <

M andr >1by Yamazaki [16]:

(a) 0≤C(m, M, r)≤M(Mr−1−mr−1)forr >1

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(b) C(m, M, r)→0asr →1 (c) C mr, Mr,1r

→L(m, M) logMh(1)asr →+0.

In the case of0 < r ≤ s ≤ 1, if we put r → 0in (iii) of Theorem 4.1, then F(r) → A♦λB and C mr, Mr,1r

→ L(m, M) logMh(1) as r → 0.

Therefore we have(i).

In the case of0 < r ≤ 1 ≤ s, if we putr → 0in(i)of Theorem4.1, then we have(ii).

As a result, we obtain an operator version of the Mond-Shisha theorem (1.2):

Theorem 4.3. LetAandB be positive operators on a Hilbert spaceH satisfy- ingm≤A, B ≤M for some scalars0< m < M andh= Mm. Then

−L(m, M) logMh(1)≤A∇λB−A♦λB ≤L(m, M) logMh(1) hold for allλ∈[0,1].

Proof. Since C(m, M, s) → 0 as s → 1, we have the conclusion by (ii) of Theorem4.2.

By combining Theorem4.3and a reverse Young inequality (1.4), we obtain an estimate of the difference between the geometric mean and the chaotically geometric one:

Corollary 4.4. LetAandB be positive operators on a Hilbert space H satis- fyingm≤A, B ≤M for some scalars0< m < M andh= Mm. Then

−(1 +h)L(m, M) logMh(1)≤A]λB−A♦λB ≤L(m, M) logMh(1) holds for allλ∈[0,1].

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Proof. SinceA]λB ≤A∇λB, it follows from Theorem4.3that A]λB−A♦λB ≤A∇λB−A♦λB ≤L(m, M) logMh(1).

By Theorem4.3and a reverse Young inequality (1.4), it follows that

−L(m, M) logMh(1) ≤A∇λB−A♦λB

≤A]λB+hL(m, M) logMh(1)−A♦λB.

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References

[1] J.I. FUJII AND Y. SEO, Determinant for positive operators, Sci. Math., 1(2) (1998), 153–156.

[2] J.I. FUJII ANDY. SEO, Characterizations of chaotic order associated with the Mond-Shisha difference, Math. Inequal. Appl., 5 (2002), 725–734.

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[8] J. MI ´CI ´C, Y. SEO, S.-E. TAKAHASHIANDM. TOMINAGA, Inequalities of Furuta and Mond-Peˇcari´c, Math. Inequal. Appl., 2 (1999), 83–111.

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Reverse Inequalities on Chaotically Geometric Mean via

Specht Ratio, II

Masatoshi Fujii, Jadranka Mi´ci´c, J. Peˇcari´cand Yuki Seo

Title Page Contents

JJ II

J I

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J. Ineq. Pure and Appl. Math. 4(2) Art. 40, 2003

[10] B. MOND AND J.E. PE ˇCARI ´C, Convex inequalities for several positive operators in Hilbert space, Indian J. Math., 35 (1993), 121–135.

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[12] O. SHISHAANDB. MOND, Bounds on difference of means, Inequalities, (O.Shisha, Ed.). Academic Press, New York, 1967, 293–308.

[13] W. SPECHT, Zur Theorie der elementaren Mittel, Math. Z., 74 (1960), 91–98.

[14] M. TOMINAGA, Specht’s ratio in the Young inequality, Sci. Math. Japon., 55 (2002), 585–588.

[15] A.M. TURING, Rounding off-errors in matrix processes, Quart. J. Mech.

Appl. Math., 1 (1948), 287–308.

[16] T. YAMAZAKI, An extension of Specht’s theorem via Kantorovich in- equality and related results, Math. Inequl. Appl., 3 (2000), 89–96.

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