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Clarkson-McCarthy Interpolated Inequalities

Cristian Conde vol. 10, iss. 1, art. 4, 2009

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CLARKSON-MCCARTHY INTERPOLATED INEQUALITIES IN FINSLER NORMS

CRISTIAN CONDE

Instituto de Ciencias

Universidad Nacional de General Sarmiento J. M. Gutierrez 1150, (1613) Los Polvorines Buenos Aires, Argentina.

EMail:cconde@ungs.edu.ar

Received: 29 August, 2008

Accepted: 14 January, 2009

Communicated by: R. Bhatia

2000 AMS Sub. Class.: Primary 46B70, 47A30; Secondary 46B20, 47B10.

Key words: p-Schatten class, Complex method, Clarkson-McCarthy inequalities.

Abstract: We apply the complex interpolation method to prove that, given two spaces Bp(n)0,a;s0, Bp(n)

1,b;s1 ofn-tuples of operators in thep-Schatten class of a Hilbert spaceH, endowed with weighted norms associated to positive and invertible op- eratorsaandbofB(H)then, the curve of interpolation(B(n)p0,a;s0, Bp(n)

1,b;s1)[t]

of the pair is given by the space ofn-tuples of operators in thept-Schatten class ofH, with the weighted norm associated to the positive invertible element γa,b(t) =a1/2(a−1/2ba−1/2)ta1/2.

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Contents

1 Introduction 3

2 Geometric Interpolation 6

3 Clarkson-Kissin Type Inequalities 12

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1. Introduction

In [6], J. Clarkson introduced the concept of uniform convexity in Banach spaces and obtained that spacesLp (or lp) are uniformly convex forp > 1 throughout the following inequalities

2

kfkpp+kgkpp

≤ kf −gkpp+kf+gkpp ≤2p−1

kfkpp+kgkpp ,

Let (B(H),k · k) denote the algebra of bounded operators acting on a complex and separable Hilbert spaceH,Gl(H)the group of invertible elements ofB(H)and Gl(H)+the set of all positive elements ofGl(H).

IfX ∈ B(H)is compact we denote by{sj(X)}the sequence of singular values ofX (decreasingly ordered). For0< p < ∞, let

kXkp =X

sj(X)pp1 ,

and the linear space

Bp(H) ={X ∈B(H) :kXkp <∞}.

For 1 ≤ p < ∞, this space is called the p−Schatten class of B(H) (to simplify notation we use Bp) and by conventionkXk = kXk = s1(X). A reference for this subject is [9].

C. McCarthy proved in [14], among several other results, the following inequali- ties forp-Schatten norms of Hilbert space operators:

2(kAkpp+kBkpp)≤ kA−Bkpp+kA+Bkpp (1.1)

≤2p−1(kAkpp+kBkpp),

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for2≤p <∞, and

2p−1(kAkpp+kBkpp)≤ kA−Bkpp+kA+Bkpp (1.2)

≤2(kAkpp+kBkpp), for1≤p≤2.

These are non-commutative versions of Clarkson’s inequalities. These estimates have been found to be very powerful tools in operator theory (in particular they imply the uniform convexity ofBpfor1< p <∞) and in mathematical physics (see [16]).

M. Klaus has remarked that there is a simple proof of the Clarkson-McCarthy in- equalities which results from mimicking the proof that Boas [4] gave of the Clarkson original inequalities via the complex interpolation method.

In a previous work [7], motivated by [1], we studied the effect of the complex interpolation method onB(n)p (this set will be defined below) forp, s≥1andn ∈N with a Finsler norm associated witha∈Gl(H)+:

kXkp,a;s:=ka−1/2Xa−1/2ksp.

From now on, for the sake of simplicity, we denote with lower case letters the ele- ments ofGl(H)+.

As a by-product, we obtain Clarkson type inequalities using the Klaus idea with the linear operatorTn:Bp(n) −→Bp(n)given by

Tn( ¯X) = (Tn(X1, . . . , Xn) =

n

X

j=1

Xj,

n

X

j=1

θ1jXj, . . . ,

n

X

j=1

θn−1j Xj

! ,

whereθ1, . . . , θnare thenroots of unity.

Recently, Kissin in [12], motivated by [3], obtained analogues of the Clarkson- McCarthy inequalities forn-tuples of operators from Schatten ideals. In this work

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the author considersHn,the orthogonal sum ofncopies of the Hilbert spaceH,and each operator R ∈ B(Hn) can be represented as an n ×n block-matrix operator R = (Rjk)withRjk ∈ B(H),and the linear operator TR : Bp(n) →Bp(n) is defined byTR(A) =RA. Finally we remark that the works [3] and [11] are generalizations of [10].

In these notes we obtain inequalities for the linear operatorTRin the Finsler norm k·kp,a;sas by-products of the complex interpolation method and Kissin’s inequalities.

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2. Geometric Interpolation

We follow the notation used in [2] and we refer the reader to [13] and [5] for de- tails on the complex interpolation method. For completeness, we recall the classical Calderón-Lions theorem.

Theorem 2.1. Let X andY be two compatible couples. Assume thatT is a linear operator fromXj toYj bounded byMj,j = 0,1. Then fort∈[0,1]

kTkX

[t]→Y[t] ≤M01−tM1t.

Here and subsequently, let1≤p < ∞, n∈N, s≥1,a∈Gl(H)+and Bp(n) ={A= (A1, . . . , An)t :Ai ∈Bp},

(where withtwe denote the transpose of then-tuple) endowed with the norm kAkp,a;s = (kA1ksp,a+· · ·+kAnksp,a)1/s,

andCnendowed with the norm

|(a0, . . . , an−1)|s = (|a0|s+· · ·+|an−1|s)1/s.

From now on, we denote withBp,a;s(n) the spaceBp(n)endowed with the normk(·, . . . ,·)kp,a;s. From Calderón-Lions interpolation theory we get that forp0, p1, s0, s1 ∈[1,∞) (2.1)

Bp(n)

0,1;s0, Bp(n)

1,1;s1

[t]

=Bp(n)t,1;st, where

1 pt

= 1−t p0

+ t p1

and 1

st

= 1−t s0

+ t s1

.

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Note that forp= 2, (1.1) and (1.2) both reduce to the parallelogram law 2(kAk22+kBk22) = kA−Bk22+kA+Bk22,

while for the casesp = 1,∞ these inequalities follow from the triangle inequality forB1 andB(H) respectively. Then the inequalities (1.1) and (1.2) can be proved (forn= 2via Theorem2.1) by interpolation between the previous elementary cases with the linear operator T2 : Bp,1;p(2) −→ Bp,1;p(2) , T2(A) = (A1 +A2, A1 −A2)t as observed by Klaus.

In this section, we generalize (2.1) for the Finsler normsk(·, . . . ,·)kp,a;s. In [7], we have obtained this extension for the particular case when p0 = p1 = p and s0 =s1 =s. For sake of completeness, we recall this result

Theorem 2.2 ([7, Th. 3.1]). Let a, b ∈ Gl(H)+,1 ≤ p, s < ∞, n ∈ N and t∈(0,1). Then

Bp,a;s(n) , Bp,b;s(n)

[t]

=B(n)p,γ

a,b(t);s, whereγa,b(t) = a1/2(a−1/2ba−1/2)ta1/2.

Remark 1. Note that whena andb commute the curve is given byγa,b(t) = a1−tbt. The previous corollary tells us that the interpolating space,Bp,γa,b(t);scan be regarded as a weightedp-Schatten space with weighta1−tbt(see [2, Th. 5.5.3]).

We observe that the curve γa,b looks formally equal to the geodesic (or shortest curve) between positive definitive matrices ([15]), positive invertible elements of a C-algebra ([8]) and positive invertible operators that are perturbations of the p- Schatten class by multiples of the identity ([7]).

There is a natural action ofGl(H)onBp(n),defined by

(2.2) l :Gl(H)×Bp(n)−→Bp(n), lg(A) = (gA1g, . . . , gAng)t.

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Proposition 2.3 ([7, Prop. 3.1]). The norm inBp,a;s(n) is invariant for the action of the group of invertible elements. By this we mean that for eachA∈ Bp(n), a ∈Gl(H)+ andg ∈Gl(H), we have

A

p,a;s = lg(A)

p,gag;s.

Now, we state the main result of this paper, the general case1≤ p0, p1, s0, s1 <

∞.

Theorem 2.4. Leta, b ∈ Gl(H)+,1 ≤ p0, p1, s0, s1 < ∞, n ∈ N andt ∈ (0,1).

Then

Bp(n)0,a;s0, Bp(n)

1,b;s1

[t]

=Bp(n)

ta,b(t);st, where

1

pt = 1−t p0 + t

p1 and 1

st = 1−t s0 + t

s1.

Proof. For the sake of simplicity, we will only consider the casen= 2and omit the transpose. The proof below works forn-tuples (n ≥3) with obvious modifications.

By the previous proposition,k(X1, X2)k[t]is equal to the norm ofa−1/2(X1, X2)a−1/2 interpolated between the norms k(·,·)kp0,1;s0 and k(·,·)kp1,c;s1. Consequently it is sufficient to prove our statement for these two norms.

Lett∈(0,1)and(X1, X2)∈Bp(2)t such thatk(X1, X2)kpt,ct;st = 1, and define g(z) =

U1

cz2ct2X1c−t2 cz2

λ(z)

, U2

cz2ct2X2ct2cz2

λ(z)

= (g1(z), g2(z)), where

λ(z) = pt

1−z p0 + z

p1

st

1−z s0 + z

s1

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andXi =Ui|Xi|is the polar decomposition ofXifori= 1,2.

Then for eachz ∈S,g(z)∈Bp(2)0 +Bp(2)1 and kg(iy)ksp0

0,1;s0 =

2

X

k=1

Uk

ciy2 ct2Xkc2tciy2

λ(iy)

s0

p0

!

2

X

k=1

ciy2ct2Xkc2tciy2

pt

pt

!

2

X

k=1

kXkkppt

t,ct

!

= 1

and

kg(1 +iy)ksp11,c;s1

2

X

k=1

kXkkppt

t,ct

!

= 1.

Since g(t) = (X1, X2) and g = (g1, g2) ∈ F

Bp(2)0,1;s0, Bp(2)1,c;s1

, we have k(X1, X2)k[t]≤1. Thus we have shown that

k(X1, X2)k[t]≤ k(X1, X2)kp

t,ct;st. To prove the converse inequality, letf = (f1, f2)∈ F

Bp(2)0,1;s0, Bp(2)1,c;s1

; f(t) = (X1, X2)and Y1, Y2 ∈ B0,0(H)(the set of finite-rank operators) with kYkkqt ≤ 1, where qt is the conjugate exponent for 1 < pt < ∞ (or a compact operator and q=∞ifp= 1). Fork = 1,2, let

gk(z) = cz2Ykcz2.

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Consider the functionh:S→ C2,|(·,·)|s

t

,

h(z) = (tr(f1(z)g1(z)), tr(f2(z)g2(z))).

Sincef(z)is analytic in

Sand bounded inS, thenhis analytic in

Sand bounded in S, and

h(t) = tr

ct2X1c2tY1 , tr

c2tX2c2tY2

= (h1(t), h2(t)).

By Hadamard’s three line theorem applied tohand the Banach space(C2,|(·,·)|st), we have

|h(t)|st ≤max

sup

y∈R

|h(iy)|st,sup

y∈R

|h(1 +iy)|st

. Forj = 0,1,

sup

y∈R

|h(j+iy)|st = sup

y∈R 2

X

k=1

|tr(fk(j +iy)gk(j+iy))|st

!st1

= sup

y∈R 2

X

k=1

|tr(c−j/2fk(j+iy)c−j/2gk(iy))|st

!st1

≤sup

y∈R 2

X

k=1

kfk(j+iy)ksp,ctj

!st1

≤ kfkF

Bp(2)

0,1;s0,B(2)p1,c;s1

,

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then

kX1kspt

t,ct +kX2kspt

t,ct = sup

kY1kqt≤1,Y1∈B00(H) kY2kqt≤1,Y2∈B00(H)

{|h1(t)|st +|h2(t)|st}

= sup

kY1kqt≤1,Y1∈B00(H) kY2kqt≤1,Y2∈B00(H)

|h(t)|sst

t ≤ kfkst

F Bp(2)

0,1;s0,B(2)p1,c;s1

.

Since the previous inequality is valid for each f ∈ F

Bp(2)0,1;s0, Bp(2)1,c;s1

with f(t) = (X1, X2), we have

k(X1, X2)kpt,ct;st ≤ k(X1, X2)k[t].

In the special case thatp0 =p1 =pands0 =s1 =swe obtain Theorem2.2.

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3. Clarkson-Kissin Type Inequalities

Bhatia and Kittaneh [3] proved that if2≤p < ∞, then n2p

n

X

j=1

kAjk2p

n

X

j=1

kBjk2p ≤n2−2p

n

X

j=1

kAjk2p.

n

n

X

j=1

kAjkpp

n

X

j=1

kBjkpp ≤np−1

n

X

j=1

kAjkpp. (for0 < p ≤ 2, these two inequalities are reversed) where Bj = Pn

k=1θjkAk with θ1, . . . , θnthenroots of unity.

If we interpolate these inequalities we obtain that

n1p

n

X

j=1

kAjkspt

!st1

n

X

j=1

kBjkspt

!st1

≤n(1−1p) Xn

j=1

kAjkspt

!st1 , where

1 st

= 1−t 2 + t

p. Dividing bynst, we obtain

n1p 1 n

n

X

j=1

kAjkspt

!st1

≤ 1 n

n

X

j=1

kBjkspt

!st1

≤n(1−1p) 1 n

n

X

j=1

kAjkspt

!st1 .

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This inequality can be rephrased as follows, ifµ∈[2, p]then

n1p 1 n

n

X

j=1

kAjkµp

!µ1

≤ 1 n

n

X

j=1

kBjkµp

!1µ

≤n(1−1p) 1 n

n

X

j=1

kAjkµp

!µ1 .

In each of the following statementsR ∈Gl(Hn)and we denote byTRthe linear operator

TR :Bp(n)−→Bp(n) TR(A) = RA= (B1, . . . , Bn)t, with Bj = Pn

k=1RjkAk and α = kR−1k, β = kRk (we use the same symbol to denote the norm inB(H)andB(Hn)).

We observe that if the norm ofTRis at mostM when TR: Bp(n),k(·, . . . ,·)kp,1,s

→ Bp(n),k(·, . . . ,·)kp,1,r

,

then if we consider the operatorTRbetween the spaces TR: Bp(n),k(·, . . . ,·)kp,a,s

→ Bp(n),k(·, . . . ,·)kp,b,r , its norm is at mostF(a, b)M with

F(a, b) =

min{kb−1kkak,ka1/2b−1a1/2kka−1kkak} ifa 6=b,

ka−1kkak if a =b.

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Remark 2. Ifa−1/2 ∈Gl(H)commutes withR ∈B(Hn), that is, ifa−1/2commutes withRjk for all1≤j, k ≤n, thenF is reduced to

F(a, b) =

min{kb−1kkak,ka1/2b−1a1/2k}=ka1/2b−1a1/2k ifa6=b,

1 if a=b.

In [12], Kissin proved the following Clarkson type inequalities for then-tuples A∈Bp(n). If2≤p <∞andλ, µ∈[2, p], or if0< p ≤2andλ, µ∈[p,2], then

n−f(p)α−1 1 n

n

X

j=1

kAjkµp

!1µ

≤ 1 n

n

X

j=1

kBjkλp

!λ1 (3.1)

≤nf(p)β 1 n

n

X

j=1

kAjkµp

!µ1 ,

wheref(p) =

1 p12

.

Remark 3. This result extends the results of Bhatia and Kittaneh proved forµ=λ= 2orpandR = (Rjk)where

Rjk =e(i2π(j−1)(k−1)

n )1.

We use the inequalities (3.1) and the interpolation method to obtain the following inequalities.

Theorem 3.1. Leta, b∈Gl(H)+, A∈Bp(n),1≤p <∞andt∈[0,1],then

(3.2) ˜k

n

X

j=1

kAjkµp,a

!1µ

n

X

j=1

kBjkλp,γ

a,b(t)

!λ1

≤K˜

n

X

j=1

kAjkµp,a

!µ1

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where

˜k= ˜k(p, a, b, t) =F(a, a)t−1F(b, a)−tnλ1µ1|p112−1, and

K˜ = ˜K(p, a, b, t) = F(a, a)1−tF(a, b)tnλ11µ+|1p12|β, if2≤pandλ, µ∈[2, p]or if1≤p≤2andλ, µ∈[p,2].

Proof. We will denote byγ(t) =γa,b(t), when no confusion can arise.

Consider the spaceB(n)p with the norm:

kAkp,a;s = (kA1ksp,a+· · ·+kAnksp,a)1/s, wherea∈Gl(H)+.

By (3.1), the norm ofTRis at mostF(a, a)n1λ1µ+|1p12|βwhen TR : Bp(n),k(·, . . . ,·)kp,a;µ

−→ Bp(n),k(·, . . . ,·)kp,a;λ , and the norm ofTRis at mostF(a, b)nλ11µ+|1p12|βwhen

TR: Bp(n),k(·, . . . ,·)kp,a;µ

−→ Bp(n),k(·, . . . ,·)kp,b;λ .

Therefore, using the complex interpolation, we obtain the following diagram of interpolation fort ∈[0,1]

(Bp(n),k(·, . . . ,·)kp,a;λ)

(Bp(n),k(·, . . . ,·)kp,a;µ) TR //

TR

**U

UU UU UU UU UU UU UU U

TR

44i

ii ii ii ii ii ii ii ii

(Bp(n),k(·, . . . ,·)kp,γ(t);λ)

(Bp(n),k(·, . . . ,·)kp,b;λ).

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By Theorem2.1,TRsatisfies

(3.3) kTR(A)kp,γ(t);λ ≤F(a, a)1−tF(a, b)tn1λ1µ+|1p12|βkAkp,a;µ. Now applying the Complex method to

(B(n)p ,k(·, . . . ,·)kp,a;λ)

TR−1

**U

UU UU UU UU UU UU UU UU

(Bp(n),k(·, . . . ,·)kp,γ(t);λ)TR−1 //(Bp(n),k(·, . . . ,·)kp,a;µ)

(Bp(n),k(·, . . . ,·)kp,b;λ)

TiRi−1iiiiiiiii44 ii

ii ii

one obtains

(3.4) kTR−1(A)kp,a;µ≤F(a, a)1−tF(b, a)tnµ1λ1+|1p12|αkAkp,γ(t);λ. Replacing in (3.4)AbyRAwe obtain

(3.5) kAkp,a;µ ≤F(a, a)1−tF(b, a)tn1µ1λ+|1p12|αkRAkp,γ(t);λ, or equivalently

(3.6) F(a, a)t−1F(b, a)−tnλ1µ1|p112−1kAkp,a;µ ≤ kTR(A)kp,γ(t);λ. Finally, the inequalities (3.3) and (3.6) complete the proof.

We remark that the previous statement is a generalization of Th. 4.1 in [7] where Tn = TR with R =

e(i2π(j−1)(k−1)

n )1

1≤j,k≤n and a−1/2 commutes with R for all a∈Gl(H)+.

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On the other hand, it is well known that ifx1, . . . , xnare non-negative numbers, s ∈ R and we denoteMs(x) = n1 Pn

i=1xsi1/s

then for 0 < s < s0, Ms(x) ≤ Ms0(x).

If we denote kBk = (kB1kp, . . . ,kBnkp) and we consider 1 < p ≤ 2, then it holds fort∈[0,1]and s1

t = 1−tp + qt that

Mst(kBk)≤ Mq(kBk)≤r2p−1β2qn−1q

n

X

j=1

kAjkpp

!1p ,

or equivalently

(3.7)

n

X

j=1

kBjkspt

!1

st

≤r2p−1β2qnst11q

n

X

j=1

kAjkpp

!1p .

Analogously, for2≤p < ∞we get

(3.8)

n

X

j=1

kAjkpp

!1p

≤ρ1−2pα2pn1qst1

n

X

j=1

kBjkspt

!st1

where s1

t = 1−tq +pt.

Now we can use the interpolation method with the inequalities (3.7) and (3.1) (or (3.8) and (3.1)).

If we consider the following diagram of interpolation with 1 < p ≤ 2 andt ∈

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[0,1],

(Bp(n),k(·, . . . ,·)kp,1;p)

(Bp(n),k(·, . . . ,·)kp,1;p) TR //

TR

**T

TT TT TT TT TT TT TT T

TR

44i

ii ii ii ii ii ii ii i

(B(n)p ,k(·, . . . ,·)kp,1;st)

(B(n)p ,k(·, . . . ,·)kp,1;q).

By Theorem2.1and (3.1),TRsatisfies

(3.9) kTR(A)kp,1;st ≤ nf(p)β1−t

r2p−1β2qt

kAkp,1;p.

Finally, from the inequalities (3.7) and (3.9) we obtain

n

X

j=1

kBjkspt

!st1

≤minn

rp2−1β2qnst11q, nf(p)(1−t)β1+t(2q−1)r(2p−1)to Xn

j=1

kAjkpp

!1p .

We can summarize the previous facts in the following statement.

Theorem 3.2. Let A ∈ Bp(n) and B = RA, where R = (Rjk) is invertible. Let r = maxkRjkk, ρ = maxk(R−1)jkkandq be the conjugate exponent of p. Then, fort ∈[0,1]we get

n

X

j=1

kAjkpp

!1p

≤minn

ρ1−2pα2pn1qst1 , nf(p)tαt+(1−t)2pρ(1−2p)(1−t)o Xn

j=1

kBjkspt

!1s t

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Clarkson-McCarthy Interpolated Inequalities

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if2≤pand s1

t = 1−tq + tp,or

n

X

j=1

kBjkspt

!st1

≤min n

rp2−1β2qnst11q, nf(p)(1−t)β1+t(2q−1)r(2p−1)t

o Xn

j=1

kAjkpp

!1p , if1< p≤2and s1

t = 1−tp +qt.

Finally using the Finsler normk(·, . . . ,·)kp,a;s, Calderón’s method and the previ- ous inequalities we obtain:

Corollary 3.3. Leta, b ∈ Gl(H)+, A ∈ Bp(n) and B = RA, whereR = (Rjk) is invertible. Letr= maxkRjkk,ρ= maxk(R−1)jkkandqbe the conjugate exponent ofp. Then, fort, u ∈[0,1]we get

n

X

j=1

kAjkpp,a

!1p

≤F(a, a)1−uF(b, a)uM1

n

X

j=1

kBjksp,γt

a,b(u)

!st1 ,

if2≤p, s1

t = 1−tq + pt and

M1 =M1(R, p, t) = minn

ρ1−2pα2pn1qst1 , nf(p)tαt+(1−t)2pρ(1−p2)(1−t)o or

n

X

j=1

kBjksp,γt

a,b(u)

!st1

≤F(a, a)1−uF(a, b)uM2

n

X

j=1

kAjkpp

!1p , if1< p≤2, s1

t = 1−tp +qt and M2 =M2(R, p, t) = minn

rp2−1β2qnst11q, nf(p)(1−t)β1+t(2q−1)r(2p−1)to .

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Clarkson-McCarthy Interpolated Inequalities

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References

[1] E. ANDRUCHOW, G. CORACH, M. MILMAN AND D. STOJANOFF, Geodesics and interpolation, Revista de la Unión Matemática Argentina, 40(3- 4) (1997), 83–91.

[2] J. BERGH AND J. LÖFSTRÖM, Interpolation Spaces. An Introduction, Springer-Verlag, New York, 1976.

[3] R. BHATIAANDF. KITTANEH, Clarkson inequalities with several operators, Bull. London Math. Soc., 36(6) (2004), 820–832.

[4] R. BOAS, Some uniformly convex spaces, Bull. Amer. Math. Soc., 46 (1940), 304–311.

[5] A. CALDERÓN, Intermediate spaces and interpolation, the complex method, Studia Math., 24 (1964), 113–190.

[6] J.A. CLARKSON, Uniformly convex spaces, Trans. Amer. Math. Soc., 40 (1936), 396–414.

[7] C. CONDE, Geometric interpolation inp-Schatten class, J. Math. Anal. Appl., 340(2) (2008), 920–931.

[8] G. CORACH, H. PORTAANDL. RECHT, The geometry of the space of self- adjoint invertible elements of a C-algebra, Integra. Equ. Oper. Theory, 16(3) (1993), 333–359.

[9] I. GOHBERG AND M. KREIN, Introduction to the Theory of Linear Non- selfadjoint Operators, American Mathematical Society, Vol. 18, Providence, R. I.,1969.

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[10] O. HIRZALLAHANDF. KITTANEH, Non-commutative Clarkson inequalities for unitarily invariants norms, Paciic J. Math., 202 (2002), 363–369.

[11] O. HIRZALLAHANDF. KITTANEH, Non-commutative Clarkson inequalities forn-tuples of operators, Integr. Equ. Oper. Theory, 60 (2008), 369–379.

[12] E. KISSIN, On Clarkson-McCarthy inequalities forn-tuples of operators, Proc.

Amer. Math. Soc., 135(8) (2007), 2483–2495.

[13] S. KREIN, J. PETUNINANDE. SEMENOV, Interpolation of linear operators.

Translations of Mathematical Monographs, Vol. 54, American Mathematical Society, Providence, R. I., 1982.

[14] C. MCCARTHY,cp, Israel J. Math., 5 (1967), 249–271.

[15] G. MOSTOW, Some new decomposition theorems for semi-simple groups, Mem. Amer. Math. Soc., 14 (1955), 31–54.

[16] B. SIMON, Trace Ideals and their Applications. Second edition, Mathematical Surveys and Monographs, 120. American Mathematical Society, Providence, RI, 2005.

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