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An equivalent quasinorm for the Lipschitz space of noncommutative martingales

  • Congbian Ma EMAIL logo and Yanbo Ren
Published/Copyright: November 21, 2020

Abstract

In this paper, an equivalent quasinorm for the Lipschitz space of noncommutative martingales is presented. As an application, we obtain the duality theorem between the noncommutative martingale Hardy space h p c ( ) (resp. h p r ( ) ) and the Lipschitz space λ β c ( ) (resp. λ β r ( ) ) for 0 < p < 1 , β = 1 p 1 . We also prove some equivalent quasinorms for h p c ( ) and h p r ( ) for p = 1 or 2 < p < .

MSC 2010: 46L53; 46L52; 60G42

1 Introduction

In the past two decades, due to the excellent work of Pisier and Xu on noncommutative martingale inequalities [1], the study of noncommutative martingale theory has attracted more and more attention. Especially in recent years, some meaningful research results on the noncommutative martingale theory have emerged continuously, and it has become a research hotspot in the field of noncommutative analysis.

The Lipschitz space was first introduced in the classical martingale theory by Herz and plays an important role in it. For instance, the Lipschitz space is the generalization of the BMO space and the dual space of the Hardy space h p ( 0 < p 1 ). The noncommutative Lipschitz spaces λ 0 c ( ) and λ 0 r ( ) were first introduced in [2], and with their help, the atomic decomposition for the Hardy space h 1 ( ) was proved. In this paper, we study the noncommutative Lipschitz spaces λ β c ( ) and λ β r ( ) for β 0 . We show that for < q < 0 , β = 1 q , we have

λ β c ( ) = X q c ( ) and λ β r ( ) = X q r ( )

with equivalent norms. As its application, we have the duality equalities for 0 < p < 1 and β = 1 p 1

( h p c ( ) ) = λ β c ( ) and ( h p r ( ) ) = λ β r ( ) .

This answers positively a question asked in [2]. The other main result of this paper concerns the equivalent quasinorms for h p c ( ) and h p r ( ) for p = 1 or 2 < p < . We prove the equalities

h 1 c ( ) = L 1 2 , c ( ) and h 1 r ( ) = L 1 2 , r ( ) ,

which give a new characterization of h 1 c ( ) and h 1 r ( ) .

This paper is organized as follows. Some definitions and notations are given in Section 2. An equivalent quasinorm for noncommutative martingale Lipschitz space is shown in Section 3. Equivalent quasinorms for h p c ( ) and h p r ( ) for p = 1 or 2 < p < are considered in Section 4.

2 Preliminaries

Let be a von Neumann algebra acting on a Hilbert space H and τ be a normal faithful finite trace on . We call , τ a noncommutative probability space. Let x be a positive operator on H. Then x admits a unique spectral decomposition: x = 0 λ d e λ ( x ) . We will often use the spectral projection e ( λ , ) ( x ) corresponding to the interval ( λ , ) . For 0 < p , let L p ( ) be the associated noncommutative L p -space. Recall that the norm on L p ( ) is defined by

x p = ( τ ( | x | p ) ) 1 p , x L p ( ) ,

where | x | = ( x x ) 1 2 is the usual modulus of x. Note that if p = , L ( ) is just with the usual operator norm. For more detailed discussions about noncommutative Banach function spaces, see [3,4,5].

Let us recall the general setup for noncommutative martingales. Let ( n ) n 1 be an increasing filtration of von Neumann subalgebras of such that the union of n ’s is weak*-dense in and n (with 0 = 1 ) the conditional expectation with respect to n . A sequence x = ( x n ) n 1 is said to be adapted if x n L 1 ( n ) for all n 1 , and predictable if x n L 1 ( n 1 ) for n 2 . A noncommutative martingale with respect to the filtration ( n ) n 1 is a sequence x = ( x n ) n 1 in L 1 ( ) such that

n ( x n + 1 ) = x n for all n 1 .

If additionally, x = ( x n ) n 1 L p ( ) for some 0 p < , we call x an L p ( ) -martingale. In this case, we set x p = sup n x n p . If x p < , then x is called a bounded L p ( ) -martingale. Note that the space of all bounded L p -martingales, equipped with p , is isometric to L p ( ) for p > 1 . This permits us to not distinguish a martingale and its final value x (if the latter exists).

Let x = ( x n ) n 1 be a noncommutative martingale with respect to ( n ) n 1 with the usual convention that 0 = 1 . Define d x n = x n x n 1 for n 1 with the usual convention that x 0 = 0 . The sequence d x = ( d x n ) n 1 is called the martingale difference sequence of x. In the sequel, for any operator x L 1 ( ) we denote x n = n ( x ) for n 1 .

Let x = ( x n ) n 1 be a finite martingale in L 2 ( ) . We set

s c , n ( x ) = k = 1 n k 1 ( | d x k | 2 ) 1 2 , s c ( x ) = n = 1 n 1 ( | d x n | 2 ) 1 2

and

s r , n ( x ) = k = 1 n k 1 ( | d x k | 2 ) 1 2 , s r ( x ) = n = 1 n 1 ( | d x n | 2 ) 1 2 .

These will be called the column and row conditioned square functions, respectively. Let 0 < p < . Define h p c ( ) (resp. h p r ( ) ) as the completion of all finite L -martingales under the (quasi) norm x h p c ( ) = s c ( x ) p (resp. x h p r ( ) = s r ( x ) p ). For p = . We define h c ( ) (resp. h r ( ) ) as the Banach space of the L -martingales x such that n = 1 n 1 ( | d x n | ) 2 (respectively n = 1 n 1 ( | d x n | ) 2 ) converge for the weak operator topology.

For more information of noncommutative martingales, see the seminal article of Pisier and Xu [3] and the sequels to it.

The main object of this paper is the noncommutative Lipschitz spaces λ β c and λ β r ( ) .

Definition 2.1

Let β 0 . Set

λ β c ( ) = { x L 2 ( ) : x λ β c ( ) < }

with

x λ β c ( ) = max sup e P 1 τ ( e ) β 1 ( x ) , sup n 1 sup e P n τ ( e ) 1 2 β τ ( e n ( | x x n | 2 ) ) 1 2 ,

where P n denotes the lattice of projections of n .

Similarly, we define

λ β r ( ) = { x L 2 ( ) : x λ β r ( ) = x λ β c ( ) < } .

The classical martingale space L 1 2 which is defined in [6] has the following noncommutative analogue.

Definition 2.2

We define

L 1 2 , c ( ) = x L 1 ( ) : x = k = 1 y k z k , y k L 2 ( m k ) , z k L 2 ( ) , m k ( z k ) = 0 and x L 1 2 , c ( ) = inf k = 1 y k 2 z k 2 < ,

where ( m k ) k 1 and ( m k ) k 1 are the subsequences of ( k ) k 1 and ( k ) k 1 , the infimum runs over all decompositions of x as above. Similarly, define

L 1 2 , r ( ) = { x L 1 ( ) : x L 1 2 , r ( ) = x L 1 2 , c ( ) < } .

It is clear that L 1 2 , c ( ) and L 1 2 , r ( ) are Banach spaces.

We will use the following definitions from [2,7].

Definition 2.3

[2] Let 0 < p 2 . Denote the index class W 1 which consists of sequences ( ω n ) n 1 such that ( ω n 2 / p 1 ) n 1 is nondecreasing with each ω n L 1 + ( n ) invertible with bounded inverse and ω n 1 1 . Define

X p c ( ) = x L 2 ( ) : x X p c ( ) = inf W 1 τ n = 1 | ω n | 1 2 / p | d x n + 1 | 2 1 2 < .

For 2 < p or p < 0 . Denote W 2 which consists of sequences ( ω n ) n 1 such that ( ω n 1 2 / p ) n 1 is nondecreasing with each ω n L 1 + ( n ) invertible with bounded inverse and ω n 1 1 . Define

X p c ( ) = x L 2 ( ) : x X p c ( ) = sup W 2 τ n = 1 | ω n | 1 2 / p | d x n + 1 | 2 1 2 < .

Similarly, define

X p r ( ) = { x L 2 ( ) : x X p r ( ) = x X p c ( ) < } .

Remark that for 2 < p , X p c ( ) can be rewritten in the following form. Given ( ω n ) n 1 W 2 , we set

g n = ω n 2 α ω n 1 2 α 1 2 , n 1 ,

where α = 1 2 1 p . It is clear that

(3.1) ( g n ) G α = u = ( u n ) n 0 : u n L α ( n ) , τ n = 1 | u n | 2 α 2 1 .

Then

x X p c ( ) = sup ( u n ) G α τ n = 1 | u n | 2 n ( | x x n | 2 ) 1 2 .

We recall the definition of the space L p ( ; ) , with 1 p . A sequence ( x n ) n 1 in L p ( ) belongs to L p ( ; ) if ( x n ) n 1 admits a factorization x n = a y n b , with a , b L 2 p ( ) and ( y n ) n 1 L ( ) . The norm of ( x n ) n 1 is then defined as

( x n ) n 1 L p ( ; ) = inf x n = a y n b { a 2 p sup n 1 y n b 2 p } .

We usually write ( x n ) n 1 L p ( ; ) = sup n + x n p .

Definition 2.4

[7] Let 2 < p < . Define the space

L p c m o ( ) = a L 2 ( ) : sup + n ( | a n ( a ) | 2 ) p 2 <

equipped with the norm

a L p c m o ( ) = max a p , sup + n ( | a n ( a ) | 2 ) p 2 1 2 .

Then ( L p c m o ( ) , L p c m o ( ) ) is a Banach space. Similarly, we set

L p r m o ( ) = { a : a L p c m o ( ) }

equipped with the norm

a L p r m o ( ) = a L p c m o ( ) .

3 An equivalent quasinorm for the Lipschitz space of noncommutative martingales

In this section, we prove the noncommutative equivalent quasinorms for Lipschitz spaces λ β c ( ) and λ β r ( ) ( β 0 ). As its application, we obtain the duality of the Hardy space h p c ( ) (resp. h p r ( ) ) and the Lipschitz space λ β c ( ) (resp. λ β r ( ) ) for 0 < p < 1 .

Theorem 3.1

For < q < 0 and β = 1 q , we have λ β c ( ) = X q c ( ) with equivalent norms. More precisely, for any x L 2 ( ) , we have

1 2 q 1 2 x X q c ( ) x λ β c ( ) x X q c ( ) .

Similarly, λ β r ( ) = X q r ( ) with the same equivalence constants.

The following Lemma is the key ingredient of our proof.

Lemma 3.2

For x λ β c ( ) ( β 0 ) , we have

(3.1) n ( | x x n | 2 ) C 2 e n τ ( e ) 2 β e n 1 ,

where C = x λ β c ( ) and n is the set consisting of all minimal projections with respect to n .

Proof

By the definition of λ β c ( ) ( β 0 ) , we have for any e n

(3.2) τ ( e n ( | x x n | 2 ) ) 1 2 C τ ( e ) 1 2 + β .

Let P be a projection with respect to n and there does not exist any minimal projections e such that e P . Let y = n ( | x x n | 2 ) P . Then for any k 1

y e 1 k , ( y ) 1 k e 1 k , ( y ) .

Thus by (3.2), we get that

1 k τ e 1 k , ( y ) 1 2 τ y e 1 k , ( y ) 1 2 = τ n ( | x x n | 2 ) P e 1 k , ( y ) 1 2 C τ e 1 k , ( y ) P 1 2 + β .

When τ ( e ( 1 k , ) ( y ) ) 0 , we have that

(3.3) 1 k τ e 1 k , ( y ) β .

Note that e ( 1 k , ) ( y ) P and P can be divided into infinite small pieces. Thus, τ ( e ( 1 k , ) ( y ) ) = 0 , which contradicts (3.3). Therefore, we obtain τ ( e ( 1 k , ) ( y ) ) = 0 for every k 1 which implies n ( | x x n | 2 ) P = 0 .

Now we prove (3.1) holds. Let e n and a = C τ ( e ) β . Let ε > 0 and e 0 = e ( ( a + ε ) 2 , ) ( n ( | x x n | 2 ) ) . Then we have that

e e 0 n ( | x x n | 2 ) ( a + ε ) 2 e 0 e .

Thus using (3.2), we get that

( a + ε ) τ ( e 0 e ) 1 2 τ ( e 0 e E n ( | x x n | 2 ) ) 1 2 a τ ( e 0 e ) 1 2 .

It is easy to see that e 0 e = 0 , which implies that e e 0 does not hold. Using the preceding result, we have that

n ( | x x n | 2 ) e 0 = 0 .

Let e 1 = e ( 0 , a 2 ) ( n ( | x x n | 2 ) ) . Then we have

n ( | x x n | 2 ) = n ( | x x n | 2 ) e 1 a 2 e 1 .

It follows that

(3.4) n ( | x x n | 2 ) e C 2 τ ( e ) 2 β e .

Note that n ( | x x n | 2 ) ( 1 e n e ) = 0 . Thus by (3.4), we have

n ( | x x n | 2 ) = n ( | x x n | 2 ) e n e C 2 e n τ ( e ) 2 β e .

The proof is complete.□

We will also need the following well-known lemma from [8].

Lemma 3.3

Let f be a function in 1 ( + ) and x , y + . Then

τ ( f ( x + y ) f ( x ) ) = τ 0 1 f ( x + t y ) y d t .

Proof of Theorem 3.1

Let x X q c ( ) and 1 α = 1 2 1 q . Fix an integer m 0 and let e be a projection with respect to m . Define

u n = e τ ( e ) 1 α , m = n ; 0 , m n .

Noting that ( u n ) n 0 G α , we have

τ ( e ) 2 α τ ( e n | x x n | 2 ) 1 2 = τ n = 1 | u n | 2 n ( | x x n | 2 ) 1 2 x X q c ( ) .

Thus, we have that x λ β c ( ) and x λ β c ( ) x X q c ( ) .

Now, let x λ β c ( ) and C = x λ β c ( ) . Let n be the set consisting of all minimal projections with respect to n . Then by Lemma 3.3, we have that

(3.5) n ( | x x n | 2 ) C 2 e n τ ( e ) 2 β e .

Let u = ( u n ) G α . Denote r n = k n | u k | 2 α 2 and r n = r n e ( 0 , ) ( r n ) . Then r n is invertible and τ ( r n ) 1 . Let r n = 0 λ d e λ be the spectral decomposition of r n . Let d μ = d τ ( e λ ) . Then we have 0 λ d μ 1 . Observe that

λ 0 ( 0 , ) μ ( λ 0 ) χ { λ 0 } ( λ ) λ 1 ,

where χ { λ 0 } ( λ ) is the characteristic function at point λ 0 . It follows that

λ 0 ( 0 , ) μ ( λ 0 ) 2 β χ { λ 0 } ( λ ) λ 2 β .

By the continuous function calculus, we have

(3.6) e n τ ( e ) 2 β e r n 2 β .

Using (3.5) and (3.6),

(3.7) τ n = 1 | u n | 2 n ( | x x n | 2 ) 1 2 C τ n = 1 | u n | 2 e n τ ( e ) 2 β e 1 2 C τ n = 1 ( r n 2 α r n 1 2 α ) r n 1 2 α 1 2 .

Applying Lemma 3.3 with f ( t ) = t α 2 , x + y = r n 2 α and x = r n 1 2 α , we obtain

τ r n 2 α r n 1 2 α r n 1 2 α τ 0 1 r n 1 2 α + t r n 2 α r n 1 2 α α 2 1 r n 2 α r n 1 2 α d t = 2 α τ ( r n r n 1 ) ,

where we have used the fact that the operator function a a α 2 1 is nonincreasing for 1 < α 2 1 0 . Taking the sum over n leads to τ n = 1 | u n | 2 n ( | x x n | 2 ) 1 2 ( 2 α ) 1 2 x λ β c ( ) . Taking supremum over all ( u n ) G α , we get

x X p c ( ) 2 α 1 2 x λ β ( ) = 1 2 p 1 2 x λ β ( ) .

The proof is complete.□

Using the dual result in Theorem 3.2 in [2], we will describe the dual space of h p ( ) ( 0 < p < 1 ) as the Lipschitz space.

Corollary 3.4

Let 0 < p < 1 and β = 1 p 1 . Then we have

( h p c ( ) ) = λ β c ( )

and

( h p r ( ) ) = λ β r ( )

with equivalent norms.

4 Equivalent quasinorms for h 1 c ( ) and h p c ( ) ( 2 < p < )

In this section, we first describe an equivalent quasinorm for h 1 c ( ) . As in the classical case, the spaces h 1 and L 1 2 are equivalent (see [6]). We will transfer this to the noncommutative martingales.

Theorem 4.1

We have that

h 1 c ( ) = L 1 2 , c ( ) a n d h 1 r ( ) = L 1 2 , r ( )

with equivalent norms.

For the proof we need the following lemmas.

Lemma 4.2

Let 1 p 2 and p be the conjugate index of p. For x , y L 2 ( ) , we have

| τ ( x y ) | 2 p 1 2 x h p c ( ) y X p c ( ) .

Proof

Let ( r n ) W 1 . Then by the Cauchy-Schwarz inequality and Lemma 3.1, we have that

τ ( x y ) = k = 1 τ d x k r k 1 1 2 1 p d y k r k 1 1 2 1 p k = 1 τ r k 1 1 2 p | d x k | 2 1 2 k = 1 τ r k 1 1 2 p | d y k | 2 1 2 x X p c ( ) y X p c ( ) 2 p 1 2 x h p c ( ) y X p c ( ) .

Note that the set G α defined in (3.1) can be reduced to the following one:

G α ˜ = finite sequences u = ( u n ) n 1 : u n L ( n ) , τ n 1 | u n | 2 α 2 1 .

Indeed, for any ( u n ) n 0 G α set

u n ( N ) = | u n | e [ 0 , N ] ( | u n | ) , n N ; 0 , n > N .

Then we have that

lim N τ n 1 | u n ( N ) | 2 n ( | x x n | 2 ) 1 2 = τ n 1 | u n | 2 n ( | x x n | 2 ) 1 2 .

Thus, the set G α can be reduced to G α ˜ .□

Lemma 4.3

Let y L 2 ( ) and 2 p . Then we have

y X p c ( ) = sup x F 2 p | τ ( x y ) | ,

where

F 2 p = x = n 1 a n b n : ( a n ) G α ˜ , n ( b n ) = 0 , τ n 1 | b n | 2 1 2 1 .

Proof

For any finite sequences ( a n ) G α ˜ , set

A a , y = τ n 1 | a n | 2 | y n | 2 1 2 ,

where y n = y y n . Then we have A a , y < and

(4.1) A a , y = A a , y 2 A a , y = τ n 1 a n y n y n a n A a , y = τ n 1 a n y n z n ,

where z n = y n a n A a , y . Note that n ( z n ) = 1 A a , y n ( y n ) a n = 0 and

τ n 1 | z n | 2 = 1 A a , y 2 τ n 1 | y n a n | 2 = 1 A a , y 2 τ n 1 | a n | 2 | y n | 2 = 1 .

Let x = n 1 a n z n . It is clear that x F 2 p and

n 1 a n z n 2 n 1 a n z n 2 sup n 1 a n n 1 z n 2 < .

Thus,

τ n 1 a n z n y n n 1 a n z n 2 n 1 y y n 2 < .

Therefore, by the definition of X p c ( ) and (4.1), we have that

y X p c ( ) = sup ( a n ) G α ˜ A a , y = sup x F 2 p τ n 1 a n z n y n = sup x F 2 p n 1 τ ( n ( a n z n ( y y n ) ) ) = sup x F 2 p n 1 τ ( a n z n y ) n 1 τ ( a n n ( z n ) y n ) = sup x F 2 p | τ ( x y ) | .

Proof of Theorem 4.1

First let x = z y and there exists n 1 such that y L 2 ( n ) , z L 2 ( ) , n ( z ) = 0 . Then we have that

(4.2) m ( z y ) = m n ( z y ) = 0 ; m n .

Thus, we have that

(4.3) m ( z y ) = m ( z ) y ; m 1 .

Using (4.2), (4.3), and the fact y L 2 ( n ) , we find

s c ( x ) 2 = k 1 k 1 | d z k y | 2 = k > n k 1 | d z k y | 2 = y k > n k 1 | d z k | 2 y .

Thus, we deduce that

x h 1 c ( ) = s c ( x ) 1 = s c ( z ) y 1 s c ( z ) 2 y 2 = z 2 y 2 .

Therefore, we get that x h 1 c ( ) x L 1 2 , c ( ) . Now we consider the general case. Let

x = k = 1 z k y k ,

where for every k 1 , y k L 2 ( m k ) , z k L 2 ( ) , and m k ( z k ) = 0 . Then by (4.3), we have that

x h 1 c ( ) = lim n k = 1 n z k y k h 1 c ( ) lim n k = 1 n z k y k h 1 c ( ) k = 1 z k 2 y k 2 .

It follows that x h 1 c ( ) x L 1 2 , c ( ) .

We turn to the converse inequality. Let x L 1 2 , c ( ) . Then by Lemma 4.2 and Lemma 4.3,

(4.4) x L 1 2 , c ( ) = sup y L 1 2 , c ( ) , y L 1 2 , c ( ) 1 | τ ( x y ) | sup y L 1 2 , c ( ) , y L 1 2 , c ( ) 1 x h 1 c ( ) y X c ( ) x h 1 c ( ) sup y L 1 2 , c ( ) , y L 1 2 , c ( ) 1 sup a F 2 p | τ ( a y ) | .

We will show

(4.5) sup a F 2 p | τ ( a y ) | sup a L 1 2 , c ( ) , a L 1 2 , c ( ) 1 | τ ( a y ) | .

Indeed, let a F 2 p . Then a can be decomposed as

(4.6) a = n 1 r n b n ,

where ( r n ) G α ˜ , n ( b n ) = 0 and ( τ ( n 1 | b n | 2 ) ) 1 2 1 . Thus, by the Cauchy-Schwarz inequality we have that

n 1 r n 2 b n 2 n 1 r n 2 2 1 2 n 1 b n 2 2 1 2 1 .

Taking the infimum as in (4.6), we obtain a L 1 2 , c ( ) and a L 1 2 , c ( ) 1 , which imply that (4.5) holds. Combining (4.4) and (4.5), we have that x L 1 2 , c ( ) x h 1 c ( ) . Thus, we have that h 1 c ( ) = L 1 2 , c ( ) .

Similarly, we have that h 1 r ( ) = L 1 2 , r ( ) . The proof of the theorem is complete.□

Let 2 < p < . Our second result of this section concerns the equivalent quasinorms for h p c ( ) and h p r ( ) .

Theorem 4.4

Let 2 < p < . Then we have

h p c ( ) = X p c ( ) = L p c m o ( )

with equivalent norms. More precisely,

x X p c ( ) x L p c m o ( ) x h p c ( ) p 2 1 2 x X p c ( ) .

Similarly,

h p r ( ) = X p r ( ) = L p r m o ( )

with equivalent norms.

Proof

Step 1: Let x X p c ( ) . Fix a positive integer N, we will show that s c , N ( x ) L p ( ) . Let 1 n N . Since the dual space of L p 2 ( n ) is L p p 2 ( n ) ,

n ( | d x n + 1 | ) 2 p 2 = sup y n L p p 2 + ( n ) y n L p p 2 ( ) 1 τ ( y n n ( | d x n + 1 | 2 ) ) .

Let w n = y n p p 2 . Then w n 0 and τ ( w n ) 1 . Thus, we have that

n ( | d x n + 1 | ) 2 p 2 = sup w n 0 , τ ( w n ) 1 τ w n 1 2 p n ( | d x n + 1 | ) 2 x X p c ( ) 2 .

Therefore, we obtain that

n = 1 N n 1 ( | d x n | ) 2 1 2 p = n = 1 N n 1 ( | d x n | ) 2 p 2 1 2 n = 1 N n 1 ( | d x n | ) 2 p 2 1 2 N x X p c ( ) < .

Assume s c , N ( x ) p = 1 . Then the sequence s c , N p ( x ) , s c , N p ( x ) , , s c , N p ( x ) , W 2 . Set s c , 0 ( x ) = 0 . Thus, we have that

x X p c ( ) 2 τ n = 1 N ( s c , N p ( x ) ) 1 2 p ( s c , n 2 ( x ) s c , n 1 2 ( x ) ) = τ s c , N p 2 ( x ) n = 1 N ( s c , n 2 ( x ) s c , n 1 2 ( x ) ) = τ ( s c , N p ( x ) ) .

It follows that

x h p c ( ) x X p c ( ) .

Now let x h p c ( ) and ( w n ) W 2 . Set s c , 0 ( x ) = 0 . Then for any n

τ k = 1 n w k 1 2 p ( s c , k + 1 2 ( x ) s c , k 2 ( x ) ) 1 2 = τ w n 1 2 p ( s c , n + 1 2 ( x ) 1 2 ( τ ( w n ) ) 1 2 p ( τ ( s c , n + 1 p ) ) 1 p s c ( x ) p .

Thus, we get that

τ k = 1 w k 1 2 p ( s c , k + 1 2 ( x ) s c , k 2 ( x ) ) 1 2 s c ( x ) p .

Therefore, the inequality x X p c ( ) x h p c ( ) holds.

Step 2: Let x h p c ( ) . Then for any n 0

n ( | x n ( x ) | 2 ) = n k = n + 1 k 1 ( | d x k | 2 ) n ( s c 2 ( x ) ) .

Thus, we have that

x L p c m o ( ) x h p c ( ) .

Now let x L p c m o ( ) ) and 1 p + 1 p = 1 . Note that

sup + ( n ( | x n ( x ) | ) 2 ) p 2 = sup n 1 τ ( n ( | x n ( x ) | ) 2 y n ) : y n L p 2 and n 1 y n p 2 1 .

Thus, we have that

x X p c ( ) = sup ( u n ) G α τ n = 1 | u n | 2 n ( | x x n | 2 1 2 sup + ( n ( | x n ( x ) | ) 2 ) p 2 x L p c m o ( ) .

The proof of the theorem is complete.□

The following is an immediate consequence of Theorem 4.4 and Theorem 3.3 in [2] (or Theorem 3.1 in [7]).

Corollary 4.5

Let 1 < p < 2 and let q be the index conjugate to p. Then

( h p c ( ) ) = h q c ( )

and

( h p r ( ) ) = h q r ( )

with equivalent norms.

Acknowledgment

This work was supported by the National Natural Science Foundation of China (11871195, 11671308, and 11471251).

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Received: 2019-12-04
Revised: 2020-05-11
Accepted: 2020-08-10
Published Online: 2020-11-21

© 2020 Congbian Ma and Yanbo Ren, published by De Gruyter

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

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  5. The non-negative spectrum of a digraph
  6. Bounds on F-index of tricyclic graphs with fixed pendant vertices
  7. Crank-Nicolson orthogonal spline collocation method combined with WSGI difference scheme for the two-dimensional time-fractional diffusion-wave equation
  8. Hardy’s inequalities and integral operators on Herz-Morrey spaces
  9. The 2-pebbling property of squares of paths and Graham’s conjecture
  10. Existence conditions for periodic solutions of second-order neutral delay differential equations with piecewise constant arguments
  11. Orthogonal polynomials for exponential weights x2α(1 – x2)2ρe–2Q(x) on [0, 1)
  12. Rough sets based on fuzzy ideals in distributive lattices
  13. On more general forms of proportional fractional operators
  14. The hyperbolic polygons of type (ϵ, n) and Möbius transformations
  15. Tripled best proximity point in complete metric spaces
  16. Metric completions, the Heine-Borel property, and approachability
  17. Functional identities on upper triangular matrix rings
  18. Uniqueness on entire functions and their nth order exact differences with two shared values
  19. The adaptive finite element method for the Steklov eigenvalue problem in inverse scattering
  20. Existence of a common solution to systems of integral equations via fixed point results
  21. Fixed point results for multivalued mappings of Ćirić type via F-contractions on quasi metric spaces
  22. Some inequalities on the spectral radius of nonnegative tensors
  23. Some results in cone metric spaces with applications in homotopy theory
  24. On the Malcev products of some classes of epigroups, I
  25. Self-injectivity of semigroup algebras
  26. Cauchy matrix and Liouville formula of quaternion impulsive dynamic equations on time scales
  27. On the symmetrized s-divergence
  28. On multivalued Suzuki-type θ-contractions and related applications
  29. Approximation operators based on preconcepts
  30. Two types of hypergeometric degenerate Cauchy numbers
  31. The molecular characterization of anisotropic Herz-type Hardy spaces with two variable exponents
  32. Discussions on the almost 𝒵-contraction
  33. On a predator-prey system interaction under fluctuating water level with nonselective harvesting
  34. On split involutive regular BiHom-Lie superalgebras
  35. Weighted CBMO estimates for commutators of matrix Hausdorff operator on the Heisenberg group
  36. Inverse Sturm-Liouville problem with analytical functions in the boundary condition
  37. The L-ordered L-semihypergroups
  38. Global structure of sign-changing solutions for discrete Dirichlet problems
  39. Analysis of F-contractions in function weighted metric spaces with an application
  40. On finite dual Cayley graphs
  41. Left and right inverse eigenpairs problem with a submatrix constraint for the generalized centrosymmetric matrix
  42. Controllability of fractional stochastic evolution equations with nonlocal conditions and noncompact semigroups
  43. Levinson-type inequalities via new Green functions and Montgomery identity
  44. The core inverse and constrained matrix approximation problem
  45. A pair of equations in unlike powers of primes and powers of 2
  46. Miscellaneous equalities for idempotent matrices with applications
  47. B-maximal commutators, commutators of B-singular integral operators and B-Riesz potentials on B-Morrey spaces
  48. Rate of convergence of uniform transport processes to a Brownian sheet
  49. Curves in the Lorentz-Minkowski plane with curvature depending on their position
  50. Sequential change-point detection in a multinomial logistic regression model
  51. Tiny zero-sum sequences over some special groups
  52. A boundedness result for Marcinkiewicz integral operator
  53. On a functional equation that has the quadratic-multiplicative property
  54. The spectrum generated by s-numbers and pre-quasi normed Orlicz-Cesáro mean sequence spaces
  55. Positive coincidence points for a class of nonlinear operators and their applications to matrix equations
  56. Asymptotic relations for the products of elements of some positive sequences
  57. Jordan {g,h}-derivations on triangular algebras
  58. A systolic inequality with remainder in the real projective plane
  59. A new characterization of L2(p2)
  60. Nonlinear boundary value problems for mixed-type fractional equations and Ulam-Hyers stability
  61. Asymptotic normality and mean consistency of LS estimators in the errors-in-variables model with dependent errors
  62. Some non-commuting solutions of the Yang-Baxter-like matrix equation
  63. General (p,q)-mixed projection bodies
  64. An extension of the method of brackets. Part 2
  65. A new approach in the context of ordered incomplete partial b-metric spaces
  66. Sharper existence and uniqueness results for solutions to fourth-order boundary value problems and elastic beam analysis
  67. Remark on subgroup intersection graph of finite abelian groups
  68. Detectable sensation of a stochastic smoking model
  69. Almost Kenmotsu 3-h-manifolds with transversely Killing-type Ricci operators
  70. Some inequalities for star duality of the radial Blaschke-Minkowski homomorphisms
  71. Results on nonlocal stochastic integro-differential equations driven by a fractional Brownian motion
  72. On surrounding quasi-contractions on non-triangular metric spaces
  73. SEMT valuation and strength of subdivided star of K 1,4
  74. Weak solutions and optimal controls of stochastic fractional reaction-diffusion systems
  75. Gradient estimates for a weighted nonlinear parabolic equation and applications
  76. On the equivalence of three-dimensional differential systems
  77. Free nonunitary Rota-Baxter family algebras and typed leaf-spaced decorated planar rooted forests
  78. The prime and maximal spectra and the reticulation of residuated lattices with applications to De Morgan residuated lattices
  79. Explicit determinantal formula for a class of banded matrices
  80. Dynamics of a diffusive delayed competition and cooperation system
  81. Error term of the mean value theorem for binary Egyptian fractions
  82. The integral part of a nonlinear form with a square, a cube and a biquadrate
  83. Meromorphic solutions of certain nonlinear difference equations
  84. Characterizations for the potential operators on Carleson curves in local generalized Morrey spaces
  85. Some integral curves with a new frame
  86. Meromorphic exact solutions of the (2 + 1)-dimensional generalized Calogero-Bogoyavlenskii-Schiff equation
  87. Towards a homological generalization of the direct summand theorem
  88. A standard form in (some) free fields: How to construct minimal linear representations
  89. On the determination of the number of positive and negative polynomial zeros and their isolation
  90. Perturbation of the one-dimensional time-independent Schrödinger equation with a rectangular potential barrier
  91. Simply connected topological spaces of weighted composition operators
  92. Generalized derivatives and optimization problems for n-dimensional fuzzy-number-valued functions
  93. A study of uniformities on the space of uniformly continuous mappings
  94. The strong nil-cleanness of semigroup rings
  95. On an equivalence between regular ordered Γ-semigroups and regular ordered semigroups
  96. Evolution of the first eigenvalue of the Laplace operator and the p-Laplace operator under a forced mean curvature flow
  97. Noetherian properties in composite generalized power series rings
  98. Inequalities for the generalized trigonometric and hyperbolic functions
  99. Blow-up analyses in nonlocal reaction diffusion equations with time-dependent coefficients under Neumann boundary conditions
  100. A new characterization of a proper type B semigroup
  101. Constructions of pseudorandom binary lattices using cyclotomic classes in finite fields
  102. Estimates of entropy numbers in probabilistic setting
  103. Ramsey numbers of partial order graphs (comparability graphs) and implications in ring theory
  104. S-shaped connected component of positive solutions for second-order discrete Neumann boundary value problems
  105. The logarithmic mean of two convex functionals
  106. A modified Tikhonov regularization method based on Hermite expansion for solving the Cauchy problem of the Laplace equation
  107. Approximation properties of tensor norms and operator ideals for Banach spaces
  108. A multi-power and multi-splitting inner-outer iteration for PageRank computation
  109. The edge-regular complete maps
  110. Ramanujan’s function k(τ)=r(τ)r2(2τ) and its modularity
  111. Finite groups with some weakly pronormal subgroups
  112. A new refinement of Jensen’s inequality with applications in information theory
  113. Skew-symmetric and essentially unitary operators via Berezin symbols
  114. The limit Riemann solutions to nonisentropic Chaplygin Euler equations
  115. On singularities of real algebraic sets and applications to kinematics
  116. Results on analytic functions defined by Laplace-Stieltjes transforms with perfect ϕ-type
  117. New (p, q)-estimates for different types of integral inequalities via (α, m)-convex mappings
  118. Boundary value problems of Hilfer-type fractional integro-differential equations and inclusions with nonlocal integro-multipoint boundary conditions
  119. Boundary layer analysis for a 2-D Keller-Segel model
  120. On some extensions of Gauss’ work and applications
  121. A study on strongly convex hyper S-subposets in hyper S-posets
  122. On the Gevrey ultradifferentiability of weak solutions of an abstract evolution equation with a scalar type spectral operator on the real axis
  123. Special Issue on Graph Theory (GWGT 2019), Part II
  124. On applications of bipartite graph associated with algebraic structures
  125. Further new results on strong resolving partitions for graphs
  126. The second out-neighborhood for local tournaments
  127. On the N-spectrum of oriented graphs
  128. The H-force sets of the graphs satisfying the condition of Ore’s theorem
  129. Bipartite graphs with close domination and k-domination numbers
  130. On the sandpile model of modified wheels II
  131. Connected even factors in k-tree
  132. On triangular matroids induced by n3-configurations
  133. The domination number of round digraphs
  134. Special Issue on Variational/Hemivariational Inequalities
  135. A new blow-up criterion for the Nabc family of Camassa-Holm type equation with both dissipation and dispersion
  136. On the finite approximate controllability for Hilfer fractional evolution systems with nonlocal conditions
  137. On the well-posedness of differential quasi-variational-hemivariational inequalities
  138. An efficient approach for the numerical solution of fifth-order KdV equations
  139. Generalized fractional integral inequalities of Hermite-Hadamard-type for a convex function
  140. Karush-Kuhn-Tucker optimality conditions for a class of robust optimization problems with an interval-valued objective function
  141. An equivalent quasinorm for the Lipschitz space of noncommutative martingales
  142. Optimal control of a viscous generalized θ-type dispersive equation with weak dissipation
  143. Special Issue on Problems, Methods and Applications of Nonlinear analysis
  144. Generalized Picone inequalities and their applications to (p,q)-Laplace equations
  145. Positive solutions for parametric (p(z),q(z))-equations
  146. Revisiting the sub- and super-solution method for the classical radial solutions of the mean curvature equation
  147. (p,Q) systems with critical singular exponential nonlinearities in the Heisenberg group
  148. Quasilinear Dirichlet problems with competing operators and convection
  149. Hyers-Ulam-Rassias stability of (m, n)-Jordan derivations
  150. Special Issue on Evolution Equations, Theory and Applications
  151. Instantaneous blow-up of solutions to the Cauchy problem for the fractional Khokhlov-Zabolotskaya equation
  152. Three classes of decomposable distributions
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