Home Mathematics N-Tuples of weighted noncommutative Orlicz space and some geometrical properties
Article Open Access

N-Tuples of weighted noncommutative Orlicz space and some geometrical properties

  • Liu Bo , Ma Zhenhua EMAIL logo , Deng Quancai EMAIL logo , Zhang Aihua and Wang Guoping
Published/Copyright: November 24, 2022

Abstract

In this article, we present a new concept named the N-tuples weighted noncommutative Orlicz space j = 1 n L p , λ ( Φ j ) ( ˜ , τ ) , where L ( Φ j ) ( ˜ , τ ) is the noncommutative Orlicz space. Based on the maximum principle, the Riesz-Thorin interpolation theorem of j = 1 n L p , λ ( Φ j ) ( ˜ , τ ) is given. As applications, we obtain the Clarkson inequality and some other geometrical properties which include the uniform convexity and uniform smoothness of noncommutative Orlicz spaces L ( Φ s ) ( ˜ , τ ) , 0 < s 1 .

MSC 2010: 46L52; 47L10; 46A80

1 Preliminaries

In the world of analysis, one of the important tools for modern mathematicians is the interpolation of operators. The first theorem regarding the interpolation of operators was proven by Marcel Riesz in 1927 [1]. In 1939, his student Olof Thorin proved a generalization of Riesz’s theorem. Although sometimes referred to as the Riesz convexity theorem, due to the way he initially stated it in [1], this theorem is usually known as the Riesz-Thorin interpolation theorem. In 1936, in order to study the uniform convexity of L p space, Clarkson gave some important inequalities which are named the Clarkson inequality [2]. In [3], the author used the noncommutative Riesz-Thorin interpolation theorem to obtain the Clarkson inequality of noncommutative L p space.

The principal objective of this article is to investigate the Riesz-Thorin interpolation theorem on noncommutative Orlicz spaces, which yields the Clarkson inequality of noncommutative L p spaces. As applications, some geometrical properties such as uniform convexity and uniform smoothness of noncommutative Orlicz space L ( Φ s ) ( ˜ , τ ) , 0 < s 1 are given.

The theory of noncommutative Orlicz spaces associated with a trace was introduced by Muratov [4] and Kunze [5]. Let be a semi-finite von Neumann algebra acting on a Hilbert space with a normal semi-finite faithful trace τ . A densely defined closed linear operator A : D ( A ) with domain D ( A ) is called affiliated with if and only if U A U = A for all unitary operators U belonging to the commutant of . Clearly, if A , then A is affiliated with . If A is a (densely defined closed) operator affiliated with and A = U A the polar decomposition, where A = ( A A ) 1 2 and U is a partial isometry, then A is said to be τ -measurable if and only if there exists a number λ 0 such that τ ( e ( λ , ) ( A ) ) < , where e [ 0 , λ ] is the spectral projection of A and τ is the trace of normal faithful and semifinite. The collection of all τ -measurable operators is denoted by ˜ . The spectral decomposition implies that a von Neumann algebra is generated by its projections. Recall that an element A + is a linear combination of mutually orthogonal projections if A = k = 1 n α k e k with α k R + and projection e k such that e k e j = 0 whenever k j [3].

Next, we recall the definition and some basic properties of noncommutative Orlicz spaces.

A function Φ : [ 0 , ) [ 0 , ] is called an Orlicz function if and only if Φ ( u ) = 0 u p ( t ) d t , where the right derivative p of Φ satisfies that p is right-continuous and nondecreasing, p ( t ) > 0 whenever t > 0 and p ( 0 ) = 0 with lim t p ( t ) = [6].

If A ˜ and Φ is an Orlicz function, one can define a corresponding space, which is named the noncommutative Orlicz space, as follows:

L Φ ( ˜ , τ ) = { A ˜ : τ ( Φ ( λ A ) ) < for some λ > 0 } .

The following Luxemburg norm could be equipped for these spaces

A ( Φ ) = inf λ > 0 : τ Φ A λ 1 .

In the case of Φ ( A ) = A p , 1 p < , L ( Φ ) ( ˜ , τ ) is nothing but the noncommutative space L p ( ˜ , τ ) = { A ˜ : τ ( A p ) < } [7] and the Luxemburg norm generated by this function is expressed by the formula:

A p = ( τ ( A p ) ) 1 p .

One can define another norm on L Φ ( ˜ , τ ) as follows:

A Φ = sup { τ ( A B ) : B L Ψ ( ˜ , τ ) and τ ( Ψ ( B ) ) 1 } ,

where Ψ : [ 0 , ) [ 0 , ] is defined by Ψ ( u ) = sup { u v Φ ( v ) : v 0 } . Here we call Ψ the complementary function of Φ . In this article, we use L ( Φ ) ( ˜ , τ ) and L Φ ( ˜ , τ ) to denote the noncommutative Orlicz spaces which are equipped with Luxemberg norm and Orlicz norm, respectively.

For more information on the theory of noncommutative Orlicz spaces we refer the reader to [4,5] and [7,8, 9,10].

2 Riesz-Thorin interpolation theorem of noncommutative Orlicz spaces

In this section, we first present a new concept named N-tuple noncommutative Orlicz spaces and then give some norm inequalities. In order to research the Riesz-Thorin interpolation theorem, an equivalent definition of the Luxemburg norm must be given. As a corollary, the Clarkson inequality of noncommutative L p space could be obtained. The main ideas of proof in this article are derived from literature [3] and [11].

Let N = be the n th von Neumann algebra direct sum of with itself. We know that N acts on the direct sum Hilbert space coordinatewise:

( A 1 , A 2 , , A n ) ( x 1 , x 2 , , x n ) = j = 1 n A j x j ,

where A j , x j , and j = 1 , 2 , n . Then N + = + + + .

We define υ : N + C by υ ( A 1 , A 2 , , A n ) = j = 1 n λ j τ ( A j ) , where λ j 0 and τ is normal semifinite faithful trace on , then υ is a weighted normal faithful normal trace on N .

Definition 2.1

Let Φ = ( Φ 1 , Φ 2 , Φ n ) be n -tuple of N -functions. For each p 1 , λ j 0 , and n -tuple of weights λ = ( λ 1 , , λ n ) , consider the following direct sum space:

j = 1 n L p , λ ( Φ j ) = { A = ( A 1 , A 2 , , A n ) : A j L ( Φ j ) ( ˜ , τ ) , 1 j n }

with norm ( Φ ) , p , λ defined as follows:

(1) A ( Φ ) , p , λ = j = 1 n λ j A j ( Φ j ) p 1 p , 1 p < , max j A j ( Φ j ) , p = ,

or the norm Φ , p , λ defined in the same way as before in which ( Φ j ) is replaced by the Orlicz norm Φ j . If Ψ j is the complementary N -function of Φ j , denote by j = 1 n L q , λ ( Ψ j ) which is equipped with ( Ψ ) , q , λ and j = 1 n L q , λ Ψ j which is equipped with Ψ , q , λ for the same weights λ = ( λ 1 , , λ n ) and q = p p 1 .

Lemma 2.1

Assuming A j = 1 n L p , λ ( Φ j ) and B j = 1 n L q , λ Ψ j , where 1 p < , we have

  1. If A j ( Φ j ) , p , λ 1 , then υ ( Φ ( A ) ) A ( Φ ) , p , λ δ 1 , where δ 1 = j = 1 n λ j 1 q .

  2. If A j ( Φ j ) , p , λ > 1 , then υ ( Φ ( A ) ) > δ 2 , where δ 2 = j = 1 n λ j p A j ( Φ j ) p 1 p .

  3. (Hölder inequality) υ ( A B ) A ( Φ ) , p , λ B Ψ , q , λ .

Proof

(1) If A j ( Φ j ) , p , λ 1 , by Proposition 3.4 of [8] and classical Hölder inequality, we then have

υ ( Φ ( A ) ) = j = 1 n λ j τ ( Φ j ( A j ) ) = j = 1 n λ j 1 q λ j 1 p τ ( Φ j ( A j ) ) j = 1 n λ j τ ( Φ j ( A j ) ) p 1 p j = 1 n λ j 1 q j = 1 n λ j A j ( Φ j ) p 1 p δ 1 = A ( Φ ) , p , λ δ 1 .

(2) If A j ( Φ j ) , p , λ > 1 , by Proposition 3.4 of [8], we have

[ υ ( Φ ( A ) ) ] p = j = 1 n λ j τ ( Φ j ( A j ) ) p > j = 1 n λ j A j ( Φ j ) p j = 1 n λ j p A j ( Φ j ) p ,

which means that

υ ( Φ ( A ) ) > j = 1 n λ j p A j ( Φ j ) p 1 p = δ 2 .

(3) By Theorem 3.3 of [8] and classical Hölder inequality, one obtain that

υ ( A B ) = j = 1 n λ j τ ( A j B j ) j = 1 n λ j 1 p + 1 q A j ( Φ j ) B j Ψ j j = 1 n λ j A j ( Φ j ) p 1 p j = 1 n λ j B j Ψ j q 1 q = A ( Φ ) , p , λ B Ψ , q , λ .

Remark 1

If Φ is 1-tuple of N -function and λ = 1 , Lemma 2.1 is exactly Theorem 3.3 and Proposition 3.4 of [8].

Theorem 2.1

If A j = 1 n L p , λ ( Φ j ) , then for 1 p < , the weighted norm ( Φ ) , p , λ is given by

A ( Φ ) , p , λ = sup υ ( A B ) : B j = 1 n L p , λ Ψ j , B Ψ , q , λ 1 .

Proof

Assume B Ψ , q , λ 1 . On one side, by (3) of Lemma 2.1, we have

υ ( A B ) A ( Φ ) , p , λ B Ψ , q , λ A ( Φ ) , p , λ .

On the other side, we may take, for simplicity, that A j 0 , A j ( Φ j ) = 1 , and j = 1 n λ j = 1 , then A ( Φ ) , p , λ = 1 .

By Proposition 3.4 of [8], for any ε > 0 one obtain that

τ [ Φ j ( ( 1 + ε ) A j ) ] ( 1 + ε ) A j ( Φ j ) = 1 + ε .

Let { e j n } n = 1 be orthogonal projections of A j and 0 < τ ( e j n ) < . If we define the operator A j m = A j ( e j 1 + e j 2 + + e j m ) ( m n ) , where A j = k = 1 n α k e j k and e j k = 0 for k > n , then A j m A j as m , and there exists an m 0 such that for m m 0 ,

υ [ Φ ( ( 1 + ε ) A m ) ] = j = 1 n λ j τ [ Φ j ( ( 1 + ε ) A j m ) ] 1 + ε 2 .

Recalling that p is the left derivative of Φ , if we set

B j m = p ( ( 1 + ε ) A j m ) 1 + τ ( Ψ j ( p ( ( 1 + ε ) A j m ) ) ) ,

then B m j = 1 n E q , λ Ψ j and B j m is bounded for each m . Moreover, by Definition 1.7 of [7] and 1.9 of [6] (Young’s inequality) we have

τ ( A j m B j m ) = τ ( A j m p ( ( 1 + ε ) λ j A j m ) ) 1 + τ ( Ψ j ( p ( ( 1 + ε ) λ j A j m ) ) ) τ ( Φ j ( A j m ) ) + τ ( Ψ j ( p ( ( 1 + ε ) A j m ) ) ) 1 + τ ( Ψ j ( p ( ( 1 + ε ) λ j A j m ) ) ) 1 + τ ( Ψ j ( p ( ( 1 + ε ) A j m ) ) ) 1 + τ ( Ψ j ( p ( ( 1 + ε ) λ j A j m ) ) ) = 1 ,

one can obtain B j m Ψ j 1 , which implies that

B m Ψ , q , λ = j = 1 n λ j B j m Ψ j q 1 q 1 ,

since j = 1 n λ j = 1 .

However, one has

sup { υ ( A B ) , B Ψ , q , λ 1 } = sup j = 1 n λ j τ ( A j B j ) : B j j = 1 n L q , λ Ψ j , B Ψ , q , λ 1 sup m m 0 j = 1 n λ j τ ( A j B j m ) : B j m j = 1 n L q , λ Ψ j , B j m Ψ j , q , λ 1 1 1 + ε sup m m 0 j = 1 n λ j τ ( ( 1 + ε ) A j m B j m ) = 1 1 + ε sup m m 0 j = 1 n λ j τ ( Φ j ( 1 + ε ) A j m ) + τ ( Ψ j ( p ( 1 + ε ) A j m ) ) 1 + τ ( Ψ j ( p ( 1 + ε ) A j m ) ) > 1 1 + ε .

Since ε > 0 is arbitrary we obtain the desired inequality.□

Definition 2.2

[12] Let Φ 1 and Φ 2 be a pair of N -functions, and 0 s 1 be fixed. Then Φ s is the uniquely defined inverse of Φ s 1 ( u ) = [ Φ 1 1 ( u ) ] 1 s [ Φ 2 1 ( u ) ] s for u 0 , where Φ i 1 is the uniquely inverse of the N -function Φ i , Φ s is called an intermediate function.

Theorem 2.2

Let Φ i = ( Φ i 1 , Φ i 2 , Φ i n ) , Q i = ( Q i 1 , Q i 2 , Q i n ) , i = 1 , 2 be n-tuples of N-functions and 0 r 1 , r 2 , t 1 , t 2 , λ = ( λ 1 , , λ n ) be given positive numbers. Next let Φ s = ( Φ s 1 , Φ s 2 , Φ s n ) , Q s = ( Q s 1 , Q s 2 , Q s n ) be the associated intermediate N-functions,

1 r s = 1 s r 1 + s r 2 , 1 t s = 1 s t 1 + s t 2 , 0 s 1 .

If T : j = 1 n L r i , λ ( Φ i j ) j = 1 n L t i , λ ( Q i j ) is a bounded linear operator with bounds K 1 , K 2 , such that T A ( Q i ) , t i , λ K i A ( Φ i ) , r i , λ , A j = 1 n L r i , λ ( Φ i j ) , i = 1 , 2 , then T is also defined on j = 1 n L r s , λ ( Φ s j ) into j = 1 n L t s , λ ( Q s j ) for all 0 s 1 and one has the bound

T A ( Q s ) , t s , λ K 1 1 s K 2 s A ( Φ s ) , r s , λ ,

where A j = 1 n L r s , λ ( Φ s j ) .

Proof

Let A = ( A 1 , A 2 , , A n ) j = 1 n L r s , λ ( Φ s j ) , B = ( B 1 , B 2 , , B n ) j = 1 n L t s , λ Ψ s j , and polar decompositions A k = U k A k , B k = V k B k where A k = j = 1 n α j e k j , B k = j = 1 n β j e k j . For convenience, we assume that A ( Φ s ) , r s , λ 1 , B Ψ s , t s , λ 1 .

For z C and k = 1 , 2 , , n , we define

A ( z ) = ( A 1 ( z ) , A 2 ( z ) , , A n ( z ) )

and

B ( z ) = ( B 1 ( z ) , B 2 ( z ) , , B n ( z ) ) ,

where

A k ( z ) = U k Φ s k [ ( Φ 1 k 1 ) 1 z ( Φ 2 k 1 ) z ] ( A k ) , B k ( z ) = V k Ψ s k [ ( Ψ 1 k 1 ) 1 z ( Ψ 2 k 1 ) z ] ( B k ) .

Then,

A k ( z ) = U k Φ s k Φ 1 k 1 j = 1 n α j e k j 1 z Φ 2 k 1 j = 1 n α j e k j z = j = 1 n Φ s k [ ( Φ 1 k 1 ( α j ) ) 1 z ( Φ 2 k 1 ( α j ) ) z ] U k e k j .

Hence, z A ( z ) is an analytic function on C with value in ˜ . The same reduction applies to B .

Now we could define a bounded entire function

H ( z ) = K 1 z 1 K 2 z υ ( B ( z ) T A ( z ) ) .

If z = i t for t R , we have

A k ( i t ) = j = 1 n Φ s k [ ( Φ 1 k 1 ( α j ) ) 1 i t ( Φ 2 k 1 ( α j ) ) i t ] U k e k j = j = 1 n Φ s k Φ 2 k 1 ( α j ) Φ 1 k 1 ( α j ) i t U k e k j j = 1 n Φ s k [ Φ 1 k 1 ( α j ) ] U k e k j = Φ s k Φ 2 k 1 Φ 1 k 1 ( A k ) i t Φ s k ( Φ 1 k 1 ( A k ) ) .

Hence,

A k ( i t ) 2 = A k ( i t ) A k ( i t ) = [ Φ s k ( Φ 1 k 1 ( A k ) ) ] 2 ,

which means

A k ( i t ) = Φ s k ( Φ 1 k 1 ( A k ) ) .

Hence, for any 1 k n we have τ ( Φ 1 k ( A k ( i t ) ) ) = τ ( Φ s k ( A k ) ) , which implies that

A j ( i t ) ( Φ 1 j ) = A j ( Φ s j )

and

υ ( Φ 1 ( A ( i t ) ) ) = j = 1 n λ j τ [ Φ 1 j [ Φ s k ( Φ 1 j 1 ( A j ) ) ] ] = λ 1 τ ( Φ s 1 ( A 1 ) ) + λ 2 τ ( Φ s 2 ( A 2 ) ) + + λ n τ ( Φ s n ( A n ) ) = υ ( Φ s ( A ) ) .

We obtain that

A ( i t ) ( Φ 1 ) , r s , λ = A ( Φ s ) , r s , λ 1 .

Similarly B ( i t ) Ψ 1 , t s , λ = B Ψ s , t s , λ 1 . Thus by (3) of Lemma 2.1 and the assumption on T , we have

υ ( B ( i t ) T A ( i t ) ) K 1 B ( i t ) Ψ 1 , t s , λ A ( i t ) ( Φ 1 ) , r s , λ K 1 .

It then follows that H ( i t ) 1 for any t R . In the same way, we could know that H ( 1 + i t ) 1 .

Therefore, by the maximum principle, for any θ C , we obtain

H ( θ ) = K 1 θ 1 K 2 θ υ ( B ( θ ) T A ( θ ) ) 1 .

Hence,

υ ( B T A ) K 1 1 θ K 2 θ .

By Theorem 2.1 we could obtain that

T A ( Q s ) , r s , λ K 1 1 θ K 2 θ A ( Φ s ) , r s , λ .

Theorem 2.3

Let Φ be an N-function and Φ s be the inverse which satisfies that Φ s 1 ( u ) = [ Φ 1 ( u ) ] 1 s [ Φ 0 1 ( u ) ] s = [ Φ 1 ( u ) ] 1 s u s 2 where 0 < s 1 and Φ 0 ( u ) = u 2 . If L ( Φ ) ( ˜ , τ ) is the noncommutative Orlicz space, then we have for A , B L ( Φ s ) ( ˜ , τ ) :

A + B ( Φ s ) 2 s + A B ( Φ s ) 2 s s 2 2 s 2 A ( Φ s ) 2 2 s + B ( Φ s ) 2 2 s 2 s 2 .

Proof

Let Φ 1 = ( Φ , Φ ) be the 2-vector of N -functions, λ = ( 1 , 1 ) , 1 r 1 and set

j = 1 2 L r 1 ( Φ ) ( ˜ , τ ) = { ( A , B ) : A , B L ( Φ ) ( ˜ , τ ) , ( A , B ) ( Φ 1 ) , r 1 < } ,

where

(2) ( A , B ) ( Φ 1 ) , r 1 = [ A ( Φ ) r 1 + B ( Φ ) r 1 ] 1 r 1 , 1 r 1 < , max { A ( Φ ) , B ( Φ ) } , r 1 = .

Take Q 1 = Φ 1 = ( Φ , Φ ) and Q 2 = Φ 2 = ( Φ 0 , Φ 0 ) where Φ 0 ( u ) = u 2 .

Set r 1 = 1 , r 2 = t 2 = 2 , and t 1 = + . Define the linear operator T : j = 1 2 L r i ( Φ i ) j = 1 2 L t i ( Q i ) by the equation T ( A , B ) = ( A + B , A B ) , we then have

T ( A , B ) ( Q 1 ) , t 1 = max { A + B ( Φ ) , A B ( Φ ) } A ( Φ ) + B ( Φ ) = K 1 ( A , B ) ( Φ 1 ) , r 1 .

Hence, K 1 = 1 and since ( Φ 0 ) = 2 , we find

T ( A , B ) ( Q 2 ) , t 2 = [ A + B 2 2 + A B 2 2 ] 1 2 = 2 [ A 2 2 + B 2 2 ] 1 2 = K 2 ( A , B ) ( Φ 2 ) , r 2 .

Thus, K 2 = 2 . Let r s and t s be given by

1 r s = 1 s r 1 + s r 2 , 1 t s = 1 s t 1 + s t 2 ,

then we have r s = 2 2 s , t s = 2 s .

By Theorem 2.2,

T ( A , B ) ( Q s ) , t s 2 s s ( A , B ) ( Φ s ) , r s ,

since K 1 1 s K 2 s = 2 s 2 .

Hence, we have

( A , B ) ( Q s ) , r s = A ( Φ s ) 2 2 s + B ( Φ s ) 2 2 s 2 s 2

and

T ( A , B ) ( Q s ) , t s = A + B ( Φ s ) 2 s + A B ( Φ s ) 2 s s 2 .

The following corollary is the Clarkson inequality of noncommutative L p space and the proof is similar to the P42 of [11].

Corollary 2.1

Suppose that 1 < p < and q = p p 1 . Then for A , B L p ( ˜ , τ ) , we have

( A + B p q + A B p q ) 1 q 2 1 q ( A p p + B p p ) 1 p , 1 < p 2 ,

and

( A + B p p + A B p p ) 1 p 2 1 p ( A p q + B p q ) 1 q , 2 p .

Proof

If 1 < p 2 , let 1 < α < p 2 and Φ ( u ) = u α , Φ 0 ( u ) = u 2 , s = 2 ( p α ) p ( 2 α ) . Then 0 < s 1 and Φ s 1 ( u ) = u 1 p or Φ s ( u ) = u p . Hence, ( Φ s ) = ( p ) and since lim α 1 2 s = p p 1 = q , lim α 1 2 s 2 = 1 p by Theorem 2.3 we obtain the first inequality.

Similarly, let 2 p < β < and Φ ( u ) = u β , Φ 0 ( u ) = u 2 , s = 2 ( β p ) p ( β 2 ) . Then 0 s 1 and Φ s ( u ) = u p , lim β 2 s = p ; lim β 2 s 2 = 1 q , by the Theorem 2.3 we obtain the second inequality.□

3 Uniform convexity and uniform smoothness

In this section, we present some geometrical properties of noncommutative Orlicz spaces which include uniform convexity and uniform smoothness.

Definition 3.1

[13] Let X be a Banach space. We define its modulus of convexity by

δ X ( ε ) = inf 1 x + y 2 : x , y X , x = y = 1 , x y = ε , 0 < ε < 2

and its modulus of smoothness by

ρ X ( t ) = sup x + t y + x t y 2 1 : x , y X , x = y = 1 , t > 0 .

X is said to be uniformly convex if δ X ( ε ) > 0 for every 2 ε > 0 , and uniformly smooth if lim t 0 ρ X ( t ) t = 0 .

Theorem 3.1

Let Φ be an N-function and Φ s be the inverse which satisfies that Φ s 1 ( u ) = [ Φ 1 ( u ) ] 1 s [ Φ 0 1 ( u ) ] s = [ Φ 1 ( u ) ] 1 s u s 2 where 0 < s 1 and Φ 0 ( u ) = u 2 , then we have for 0 < ε 2 ,

δ L ( Φ s ) ( ε ) 1 1 2 2 2 s ε 2 s s 2

and

ρ L ( Φ s ) ( t ) 1 + t 2 2 s 2 s 2 1 .

Proof

First, if A B ( Φ s ) = ε , then Theorem 2.3 implies for A , B L ( Φ s ) ( ˜ , τ ) ,

A + B ( Φ s ) 2 s + ε 2 s s 2 2 s 2 2 2 s 2 = 2 .

Hence,

1 1 2 A + B ( Φ s ) 1 1 2 2 2 s ε 2 s s 2 .

Taking infimum of A ( Φ s ) = B ( Φ s ) = 1 we can obtain the desired result and L ( Φ s ) ( ˜ , τ ) is uniformly convex if 0 < ε 2 and reflexive.

Second, if A ( Φ s ) = B ( Φ s ) = 1 , then since 2 s 2 ,

1 2 ( A + t B ( Φ s ) + A t B ( Φ s ) ) 2 s 1 2 A + t B ( Φ s ) 2 s + A t B ( Φ s ) 2 s 1 2 2 s 2 A ( Φ s ) 2 2 s + t B ( Φ s ) 2 2 s 2 s 2 2 s = 1 2 2 s 2 1 + t 2 2 s 2 s 2 2 s = 1 + t 2 2 s 2 s s .

Hence,

1 2 ( A + t B ( Φ s ) + A t B ( Φ s ) ) 1 1 + t 2 2 s 2 s 2 1 .

Taking the supremum on the left we can obtain the conclusion. Since t > 0 , we have that L ( Φ s ) ( ˜ , τ ) is uniformly smooth.□

From corollary 2.1, we can easily obtain the following result which appeared in [3].

Corollary 3.1

Suppose that 1 < p < , q = p p 1 , 0 < ε , and t > 0 . Then for A , B L p ( ˜ , τ ) , we have

  1. If 1 < p < 2 , then

    δ L p ( ε ) ε q q 2 q and ρ L p ( t ) t p p .

  2. If 2 < p < , then

    δ L p ( ε ) ε p p 2 p and ρ L p ( t ) t q q .

  3. L p ( ˜ , τ ) is uniformly convex and uniformly smooth. Consequently, it is reflexive.

Acknowledgements

We want to express our gratitude to the referee for all his/her careful revision and suggestions which have improved the final version of this work.

  1. Funding information: The research has been supported by Research project of basic scientific research business expenses of provincial colleges and universities in Hebei Province (2021QNJS11), Innovation and improvement project of academic team of Hebei University of Architecture Mathematics and Applied Mathematics (No. TD202006), Nature Science Foundation of Hebei Province under (No. A2019404009), China Postdoctoral Science Foundation (No. 2019M661047), Postdoctoral Foundation of Heibei Province under Grant B2019003016, Science and Technology project of Hebei China Tobacco Industry Co., Ltd. (HBZY2022A027), Science and technology project of Hebei China Tobacco Industry Co., Ltd. (HBZY2022A024).

  2. Conflict of interest: The authors state no conflict of interest.

  3. Data availability statement: No data, models, or code were generated or used during the study.

References

[1] M. Riesz, Sur les maxima des formes bilinéaires et sur les fonctionnelles linéaires, Acta Math. 49 (1926), no. 3–4, 465–497, https://doi.org/10.1007/BF02564121. Search in Google Scholar

[2] J. A. Clarkson, Uniformly convex spaces, Trans. Amer. Math. Soc. 40 (1936), no. 3, 396–414, https://doi.org/10.2307/1989630. Search in Google Scholar

[3] Q. Xu, T. X. D. Bieke, and Z. Chen, Introduction to operator algebras and noncommutative Lp Spaces, Science Press, Beijing, 2010. Search in Google Scholar

[4] M. Muratov, Noncommutative Orlicz spaces, Dokl. Akad. Nauk Resp. Uzb. 6 (1978), 11–13. Search in Google Scholar

[5] W. Kunze, Noncommutative Orlicz spaces and generalized Arens algebras, Math. Nachr. 147 (1990), no. 1, 123–138, https://doi.org/10.1002/mana.19901470114. Search in Google Scholar

[6] S. T. Chen, Geometry of Orlicz spaces, Dissertationes Mathematicae, Institute of Mathematics Polish Academy of Sciences, Warszawa, 1996. Search in Google Scholar

[7] L. N. Jiang and Z. H. Ma, Closed subspaces and some basic topological properties of noncommutative Orlicz spaces, Proc. Math. Sci. 127 (2017), no. 3, 525–536, https://doi.org/10.1007/s12044-017-0334-7. Search in Google Scholar

[8] G. Sadeghi, Non-commutative Orlicz spaces associated to a modular on τ-measurable operators, J. Math. Anal. Appl. 395 (2012), no. 2, 705–715, https://doi.org/10.1016/j.jmaa.2012.05.054. Search in Google Scholar

[9] M. H. A. Al-Rashed and B. Zegarliński, Noncommutative Orlicz spaces associated to a state, Studia Math. 180 (2007), no. 3, 199–209, https://doi.org/10.4064/sm180-3-1. Search in Google Scholar

[10] M. H. A. Al-Rashed and B. Zegarliński, Noncommutative Orlicz spaces associated to a state II, Linear Algebra Appl. 435 (2011), no. 12, 2999–3013, https://doi.org/10.1016/j.laa.2010.10.027. Search in Google Scholar

[11] M. M. Rao and Z. D. Ren, Theory of Orlicz Spaces, Marcel Dekker Inc., New York, 1991. Search in Google Scholar

[12] C. E. Cleaver, On the extension of Lipschitz-Holder maps on Orlicz spaces, Studia Math. 42 (1972), no. 3, 195–204, https://doi.org/10.4064/sm-42-3-195-204. Search in Google Scholar

[13] J. Lindenstrauss and L. Tzafriri, Classical Banach Spaces II: Function Spaces, Springer-Verlag, Berlin, 1979. 10.1007/978-3-662-35347-9Search in Google Scholar

Received: 2022-05-06
Revised: 2022-10-24
Accepted: 2022-10-24
Published Online: 2022-11-24

© 2022 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Articles in the same Issue

  1. Regular Articles
  2. A random von Neumann theorem for uniformly distributed sequences of partitions
  3. Note on structural properties of graphs
  4. Mean-field formulation for mean-variance asset-liability management with cash flow under an uncertain exit time
  5. The family of random attractors for nonautonomous stochastic higher-order Kirchhoff equations with variable coefficients
  6. The intersection graph of graded submodules of a graded module
  7. Isoperimetric and Brunn-Minkowski inequalities for the (p, q)-mixed geominimal surface areas
  8. On second-order fuzzy discrete population model
  9. On certain functional equation in prime rings
  10. General complex Lp projection bodies and complex Lp mixed projection bodies
  11. Some results on the total proper k-connection number
  12. The stability with general decay rate of hybrid stochastic fractional differential equations driven by Lévy noise with impulsive effects
  13. Well posedness of magnetohydrodynamic equations in 3D mixed-norm Lebesgue space
  14. Strong convergence of a self-adaptive inertial Tseng's extragradient method for pseudomonotone variational inequalities and fixed point problems
  15. Generic uniqueness of saddle point for two-person zero-sum differential games
  16. Relational representations of algebraic lattices and their applications
  17. Explicit construction of mock modular forms from weakly holomorphic Hecke eigenforms
  18. The equivalent condition of G-asymptotic tracking property and G-Lipschitz tracking property
  19. Arithmetic convolution sums derived from eta quotients related to divisors of 6
  20. Dynamical behaviors of a k-order fuzzy difference equation
  21. The transfer ideal under the action of orthogonal group in modular case
  22. The multinomial convolution sum of a generalized divisor function
  23. Extensions of Gronwall-Bellman type integral inequalities with two independent variables
  24. Unicity of meromorphic functions concerning differences and small functions
  25. Solutions to problems about potentially Ks,t-bigraphic pair
  26. Monotonicity of solutions for fractional p-equations with a gradient term
  27. Data smoothing with applications to edge detection
  28. An ℋ-tensor-based criteria for testing the positive definiteness of multivariate homogeneous forms
  29. Characterizations of *-antiderivable mappings on operator algebras
  30. Initial-boundary value problem of fifth-order Korteweg-de Vries equation posed on half line with nonlinear boundary values
  31. On a more accurate half-discrete Hilbert-type inequality involving hyperbolic functions
  32. On split twisted inner derivation triple systems with no restrictions on their 0-root spaces
  33. Geometry of conformal η-Ricci solitons and conformal η-Ricci almost solitons on paracontact geometry
  34. Bifurcation and chaos in a discrete predator-prey system of Leslie type with Michaelis-Menten prey harvesting
  35. A posteriori error estimates of characteristic mixed finite elements for convection-diffusion control problems
  36. Dynamical analysis of a Lotka Volterra commensalism model with additive Allee effect
  37. An efficient finite element method based on dimension reduction scheme for a fourth-order Steklov eigenvalue problem
  38. Connectivity with respect to α-discrete closure operators
  39. Khasminskii-type theorem for a class of stochastic functional differential equations
  40. On some new Hermite-Hadamard and Ostrowski type inequalities for s-convex functions in (p, q)-calculus with applications
  41. New properties for the Ramanujan R-function
  42. Shooting method in the application of boundary value problems for differential equations with sign-changing weight function
  43. Ground state solution for some new Kirchhoff-type equations with Hartree-type nonlinearities and critical or supercritical growth
  44. Existence and uniqueness of solutions for the stochastic Volterra-Levin equation with variable delays
  45. Ambrosetti-Prodi-type results for a class of difference equations with nonlinearities indefinite in sign
  46. Research of cooperation strategy of government-enterprise digital transformation based on differential game
  47. Malmquist-type theorems on some complex differential-difference equations
  48. Disjoint diskcyclicity of weighted shifts
  49. Construction of special soliton solutions to the stochastic Riccati equation
  50. Remarks on the generalized interpolative contractions and some fixed-point theorems with application
  51. Analysis of a deteriorating system with delayed repair and unreliable repair equipment
  52. On the critical fractional Schrödinger-Kirchhoff-Poisson equations with electromagnetic fields
  53. The exact solutions of generalized Davey-Stewartson equations with arbitrary power nonlinearities using the dynamical system and the first integral methods
  54. Regularity of models associated with Markov jump processes
  55. Multiplicity solutions for a class of p-Laplacian fractional differential equations via variational methods
  56. Minimal period problem for second-order Hamiltonian systems with asymptotically linear nonlinearities
  57. Convergence rate of the modified Levenberg-Marquardt method under Hölderian local error bound
  58. Non-binary quantum codes from constacyclic codes over 𝔽q[u1, u2,…,uk]/⟨ui3 = ui, uiuj = ujui
  59. On the general position number of two classes of graphs
  60. A posteriori regularization method for the two-dimensional inverse heat conduction problem
  61. Orbital stability and Zhukovskiǐ quasi-stability in impulsive dynamical systems
  62. Approximations related to the complete p-elliptic integrals
  63. A note on commutators of strongly singular Calderón-Zygmund operators
  64. Generalized Munn rings
  65. Double domination in maximal outerplanar graphs
  66. Existence and uniqueness of solutions to the norm minimum problem on digraphs
  67. On the p-integrable trajectories of the nonlinear control system described by the Urysohn-type integral equation
  68. Robust estimation for varying coefficient partially functional linear regression models based on exponential squared loss function
  69. Hessian equations of Krylov type on compact Hermitian manifolds
  70. Class fields generated by coordinates of elliptic curves
  71. The lattice of (2, 1)-congruences on a left restriction semigroup
  72. A numerical solution of problem for essentially loaded differential equations with an integro-multipoint condition
  73. On stochastic accelerated gradient with convergence rate
  74. Displacement structure of the DMP inverse
  75. Dependence of eigenvalues of Sturm-Liouville problems on time scales with eigenparameter-dependent boundary conditions
  76. Existence of positive solutions of discrete third-order three-point BVP with sign-changing Green's function
  77. Some new fixed point theorems for nonexpansive-type mappings in geodesic spaces
  78. Generalized 4-connectivity of hierarchical star networks
  79. Spectra and reticulation of semihoops
  80. Stein-Weiss inequality for local mixed radial-angular Morrey spaces
  81. Eigenvalues of transition weight matrix for a family of weighted networks
  82. A modified Tikhonov regularization for unknown source in space fractional diffusion equation
  83. Modular forms of half-integral weight on Γ0(4) with few nonvanishing coefficients modulo
  84. Some estimates for commutators of bilinear pseudo-differential operators
  85. Extension of isometries in real Hilbert spaces
  86. Existence of positive periodic solutions for first-order nonlinear differential equations with multiple time-varying delays
  87. B-Fredholm elements in primitive C*-algebras
  88. Unique solvability for an inverse problem of a nonlinear parabolic PDE with nonlocal integral overdetermination condition
  89. An algebraic semigroup method for discovering maximal frequent itemsets
  90. Class-preserving Coleman automorphisms of some classes of finite groups
  91. Exponential stability of traveling waves for a nonlocal dispersal SIR model with delay
  92. Existence and multiplicity of solutions for second-order Dirichlet problems with nonlinear impulses
  93. The transitivity of primary conjugacy in regular ω-semigroups
  94. Stability estimation of some Markov controlled processes
  95. On nonnil-coherent modules and nonnil-Noetherian modules
  96. N-Tuples of weighted noncommutative Orlicz space and some geometrical properties
  97. The dimension-free estimate for the truncated maximal operator
  98. A human error risk priority number calculation methodology using fuzzy and TOPSIS grey
  99. Compact mappings and s-mappings at subsets
  100. The structural properties of the Gompertz-two-parameter-Lindley distribution and associated inference
  101. A monotone iteration for a nonlinear Euler-Bernoulli beam equation with indefinite weight and Neumann boundary conditions
  102. Delta waves of the isentropic relativistic Euler system coupled with an advection equation for Chaplygin gas
  103. Multiplicity and minimality of periodic solutions to fourth-order super-quadratic difference systems
  104. On the reciprocal sum of the fourth power of Fibonacci numbers
  105. Averaging principle for two-time-scale stochastic differential equations with correlated noise
  106. Phragmén-Lindelöf alternative results and structural stability for Brinkman fluid in porous media in a semi-infinite cylinder
  107. Study on r-truncated degenerate Stirling numbers of the second kind
  108. On 7-valent symmetric graphs of order 2pq and 11-valent symmetric graphs of order 4pq
  109. Some new characterizations of finite p-nilpotent groups
  110. A Billingsley type theorem for Bowen topological entropy of nonautonomous dynamical systems
  111. F4 and PSp (8, ℂ)-Higgs pairs understood as fixed points of the moduli space of E6-Higgs bundles over a compact Riemann surface
  112. On modules related to McCoy modules
  113. On generalized extragradient implicit method for systems of variational inequalities with constraints of variational inclusion and fixed point problems
  114. Solvability for a nonlocal dispersal model governed by time and space integrals
  115. Finite groups whose maximal subgroups of even order are MSN-groups
  116. Symmetric results of a Hénon-type elliptic system with coupled linear part
  117. On the connection between Sp-almost periodic functions defined on time scales and ℝ
  118. On a class of Harada rings
  119. On regular subgroup functors of finite groups
  120. Fast iterative solutions of Riccati and Lyapunov equations
  121. Weak measure expansivity of C2 dynamics
  122. Admissible congruences on type B semigroups
  123. Generalized fractional Hermite-Hadamard type inclusions for co-ordinated convex interval-valued functions
  124. Inverse eigenvalue problems for rank one perturbations of the Sturm-Liouville operator
  125. Data transmission mechanism of vehicle networking based on fuzzy comprehensive evaluation
  126. Dual uniformities in function spaces over uniform continuity
  127. Review Article
  128. On Hahn-Banach theorem and some of its applications
  129. Rapid Communication
  130. Discussion of foundation of mathematics and quantum theory
  131. Special Issue on Boundary Value Problems and their Applications on Biosciences and Engineering (Part II)
  132. A study of minimax shrinkage estimators dominating the James-Stein estimator under the balanced loss function
  133. Representations by degenerate Daehee polynomials
  134. Multilevel MC method for weak approximation of stochastic differential equation with the exact coupling scheme
  135. Multiple periodic solutions for discrete boundary value problem involving the mean curvature operator
  136. Special Issue on Evolution Equations, Theory and Applications (Part II)
  137. Coupled measure of noncompactness and functional integral equations
  138. Existence results for neutral evolution equations with nonlocal conditions and delay via fractional operator
  139. Global weak solution of 3D-NSE with exponential damping
  140. Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part I)
  141. Ground state solutions of nonlinear Schrödinger equations involving the fractional p-Laplacian and potential wells
  142. A class of p1(x, ⋅) & p2(x, ⋅)-fractional Kirchhoff-type problem with variable s(x, ⋅)-order and without the Ambrosetti-Rabinowitz condition in ℝN
  143. Jensen-type inequalities for m-convex functions
  144. Special Issue on Problems, Methods and Applications of Nonlinear Analysis (Part III)
  145. The influence of the noise on the exact solutions of a Kuramoto-Sivashinsky equation
  146. Basic inequalities for statistical submanifolds in Golden-like statistical manifolds
  147. Global existence and blow up of the solution for nonlinear Klein-Gordon equation with variable coefficient nonlinear source term
  148. Hopf bifurcation and Turing instability in a diffusive predator-prey model with hunting cooperation
  149. Efficient fixed-point iteration for generalized nonexpansive mappings and its stability in Banach spaces
Downloaded on 7.12.2025 from https://www.degruyterbrill.com/document/doi/10.1515/math-2022-0524/html
Scroll to top button