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n-quasi-A-(m,q)-isometry on a Banach space

  • In this paper, we introduce the class of n-quasi-A-(m,q)-isometry operators on a Banach space X, which represents a generalization of the n-quasi-(m,q)-isometry on a Banach space and the n-quasi-(A,m)-isometry on a Hilbert space. After giving some basic properties of this class of operators, we study the product and the power of such operators in this class.

    Citation: Khadija Gherairi, Zayd Hajjej, Haiyan Li, Hedi Regeiba. n-quasi-A-(m,q)-isometry on a Banach space[J]. AIMS Mathematics, 2023, 8(12): 28308-28321. doi: 10.3934/math.20231448

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  • In this paper, we introduce the class of n-quasi-A-(m,q)-isometry operators on a Banach space X, which represents a generalization of the n-quasi-(m,q)-isometry on a Banach space and the n-quasi-(A,m)-isometry on a Hilbert space. After giving some basic properties of this class of operators, we study the product and the power of such operators in this class.



    The class of m-isometry operators was introduced in 1990 by Agler in [1] and was developed in 1995 by Agler and Stankas in [2,3,4]. A bounded linear operator TL(H) on a Hilbert space H is called an m-isometry, for a positif integer m (that is m1), if

    βm(T):=mk=0(1)k(mk)TkTk=0,

    where T denotes the adjoint operator of T. This latter is equivalent to

    Δm(T,x):=mk=0(1)k(mk)Tkx2=0, xH.

    Some generalizations of this class of operators exist in the literature, like the (A,m)-isometry, which was introduced in 2012 by Saddi and Sid Ahmed [9], for a positif operator A, by

    βm(T,A):=mk=0(1)k(mk)TkATk=0

    or equivalently

    Δm(T,A,x):=mk=0(1)k(mk)A12Tkx2=0, xH.

    We also mention the class of n-quasi-m-isometry on a Hilbert space defined by

    βm,n(T):=mk=0(1)k(mk)Tk+nTk+n=0

    or in an equivalent manner

    Δm,n(T,x):=mk=0(1)k(mk)Tn+kx2=0, xH.

    For more details about these class, please see references [10,11].

    The n-quasi-(A,m)-isometries (which are particular cases of n-quasi-(m,q)-isometries) were thoroughly studied by Agler and Stankus in a series of three papers in which the authors employed the theory of periodic distributions to derive a function theory model for m-isometrics, a disconjugacy theory for a subclass of Toeplitz operators. In addition, they introduced a class of 2-isometrics operators arising from a class of non stationary stochastic processes related to Brownian motion.

    Recently, Sid Ahmed et al. [7] combined these two classes and introduced the n-quasi-(A,m)-isometry on a Hilbert space. Noting that all these works are in a Hilbert space H, a generalization of those on a Banach space X was developed. For example, we can mention the work of Bayart [5], who introduced the (m,q)-isometry, for an integer q1, by

    Δqm(T):=mk=0(1)k(mk)Tkxq=0, xX.

    For q=2, the (m,2)-isometry coincide with the m-isometry defined on a Hilbert space.

    We recall that the (A,m)-isometry was first introduced by Duggal in [6], for any operator AL(X), by

    Δqm(T,A,x):=mk=0(1)k(mk)ATkxq=0, xX.

    In this paper, we will generalize this last class by introducing the n-quasi-A-(m,q)-isometry on a Banach space and present some properties of this class like the product and the powers.

    The main motivation for developing this work lies in the fact of knowing whether the different properties (spectral, product and power) of the n- quasi-(m,q)-isometry on a Banach space and the n-quasi-(A,m)-isometry on a Hilbert space are valid for operators in the new generalized class introduced in Definition 2.1. Note that in our study, we remove the condition of positivity on the operator A, which exists in the Hilbert case.

    The paper is organized as follows. In Section 2, we define our class of n-quasi-A-(m,q)-isometry operators and present its basic properties. The power and the product of such operator belonging to this class are discussed in the last section.

    In this section, we define our new class and give its basic properties.

    Given a Banach space X, we denote by L(X) the class of all the (linear bounded) operators on X. Hereafter, I=IX, R(T) and σap(T) denote the identity operator, the range and the approximate spectrum of an operator TL(X), respectively. We define the class of n-quasi-A-(m,q)-isometry operators by:

    Definition 2.1. Let A,TL(X). T is called n-quasi-A-(m,q)-isometry if and only if

    Qqm,n(T,A,x):=mk=0(1)mk(mk)ATn+kxq=0, xX.

    Remark 2.1. Let A,TL(X). Then T is a n-quasi-A-(m,q)-isometry if and only if T is a A-(m,q)-isometry on ¯R(Tn).

    Indeed, T is a n-quasi-A-(m,q)-isometry if and only if

    0=mk=0(1)mk(mk)ATn+kxq, xX=mk=0(1)mk(mk)ATkTnxq, xX=mk=0(1)mk(mk)ATkyq, y¯R(Tn).

    In the following proposition, we give some spectral properties of the n-quasi-A-(m,q)-isometry operators.

    Proposition 2.1. Let A,TL(X) such that T is a n-quasi-A-(m,q)-isometry. If 0σap(A), then σap(T)=ζ(0,1){0}, where

    ζ(0,1)={xX, x=1}.

    Proof. Let (xp)p such that xp=1 and limp(TλI)xp=0.

    Since T is a n-quasi-A-(m,q)-isometry, then

    0=mk=0(1)mk(mk)ATn+kxpq=mk=0(1)mk(mk)A(Tn+kλn+k)xp+Aλn+kxpq.

    As limp(TλI)xp=0, then limp(Tn+kλn+kI)xp=0, for all k=0,1,,m.

    Therefore

    0=limpmk=0(1)mk(mk)Aλn+kxpq=|λ|nqmk=0(1)mk(mk)(|λ|q)klimpAxpq=|λ|nq(|λ|q1)mlimpAxpq.

    Since 0σap(A), then λ=0 or |λ|=1.

    Proposition 2.2. Let A,TL(X). If T is an n-quasi-A-(m,q)-isometry, then T is a n1-quasi-A-(m,q)-isometry, for all n1n.

    Proof. Let T be a n-quasi-A-(m,q)-isometry on X. By Remark 2.1, T is a A-(m,q)-isometry on ¯R(Tn). Since ¯R(Tn)¯R(Tn1) for all n1n, therefore T is a A-(m,q)-isometry on ¯R(Tn1). According to Remark 2.1, we obtain that T is a n1-quasi-A-(m,q)-isometry, for all n1n.

    In the following proposition, thanks to a suitable condition, we give the inverse sense of the Proposition 2.2.

    Proposition 2.3. Let 1pn1 such that ¯R(Tp)=¯R(Tp+1). If T is a n-quasi-A-(m,q)-isometry, then T is a p-quasi-A-(m,q)-isometry.

    Proof. Thanks to the hypothesis ¯R(Tp)=¯R(Tp+1), it follows that ¯R(Tp)=¯R(Tn). Since T is a n-quasi-A-(m,q)-isometry on X, then T is a A-(m,q)-isometry on ¯R(Tn)=¯R(Tp). Therefore, T is a p-quasi-A-(m,q)-isometry.

    As in the Hilbert case, we have the following result.

    Proposition 2.4. Let TL(X) be a n-quasi-A-(m,q)-isometry. Then T is a n-quasi-A-(,q)-isometry for all m.

    Proof.

    Qqm+1,n(T,A,x)=m+1k=0(1)m+1k(m+1k)ATn+kxq=(1)m+1ATnxq+ATn+m+1xq+mk=1(1)m+1k[(mk)+(mk1)]ATn+kxq=(1)mATnxqmk=1(1)mk(mk)ATn+kxq+mk=1(1)m+1k(mk1)ATn+kxq+ATn+m+1xq=Qqm,n(T,A,x)+m1k=0(1)mk(mk)ATn+1+kxq+ATn+1+mxq=Qqm,n+1(T,A,x)Qqm,n(T,A,x)=0.

    Example 2.1. Let T,AL(X), where X=q(N), defined by

    Tαn=wnαn and Aαn=αn+1,

    where wn=(n+1n)1q. By simple calculations, we get that T is a 2-quasi-A-(2,q)-isometry but it is not a 2-quasi-A-(1,q)-isometry. Indeed, we have

    Qq2,2(T,A,αn)=AT4αnq2AT3αnq+AT2αnq=n1(|wnwn+1wn+2wn+4|q2|wnwn+1wn+2|q+|wnwn+1|q)|αn+1|q=n1(n+4n2n+3n+n+2n)|αn+1|q=0,

    and

    Qq1,2(T,A,αn)=AT3αnqAT2αnq=n1(|wnwn+1wn+2|q|wnwn+1|q)|αn+1|q=n1(n+3nn+2n)|αn+1|q=n1|αn+1|qn0.

    Proposition 2.5. Let A,TL(X) such that T is a n-quasi-A-(m,q)-isometry. Then, for all p0, we have

    (1) ATn+pxq=m1k=0(pk)Qqk,n(T,A,x).

    (2) Qqm1,n(T,A,x)=limpATn+pxq(pm1)0.

    Proof. (1) By induction, we prove that, for all p0,

    ATn+pxq=pk=0(pk)Qqk,n(T,A,x).

    For p=0, we infer that

    0k=0(0k)Qqk,n(T,A,x)=Qq0,n(T,A,x)=ATnxq.

    We suppose that ATn+jxq=jk=0(jk)Qqk,n(T,A,x) for all jp.

    We know that

    ATn+p+1xq=Qqp+1,n(T,A,x)pk=0(1)p+1k(p+1k)ATn+kxq=Qqp+1,n(T,A,x)pk=0(1)p+1k(p+1k)kj=0(kj)Qqj,n(T,A,x)=Qqp+1,n(T,A,x)pj=0Qqj,n(T,A,x)pk=j(1)p+1k(p+1k)(kj)=Qqp+1,n(T,A,x)pj=0(p+1j)Qqj,n(T,A,x)pk=j(1)p+1k(p+1jkj)=1=Qqp+1,n(T,A,x)+pj=0(p+1j)Qqj,n(T,A,x)=p+1j=0(p+1j)Qqj,n(T,A,x).

    Then, for all p0, we have that ATn+pxq=pk=0(pk)Qqk,n(T,A,x).

    Since T is a n-quasi-A-(m,q)-isometry on X, then, by Proposition 2.4, we obtain that

    Qqk,n(T,A,x)=0,  for all km.

    Hence, for all p0, we get that

    ATn+pxq=m1k=0(pk)Qqk,n(T,A,x).

    (2) We know, by assertion (1), that

    ATn+pxq=m1k=0(pk)Qqk,n(T,A,x)=(pm1)Qqm1,n(T,A,x)+m2k=0(pk)Qqk,n(T,A,x).

    Dividing both sides by (pm1)0, we see that

    Qqm1,n(T,A,x)=1(pm1)ATn+pxq1(pm1)m2k=0(pk)Qqk,n(T,A,x).

    Upon taking the limit as p, we know that limp(pk)(pm1)=0, for all k=0,1,...,m2. Therefore, since ATn+pxq0, it holds that

    Qqm1,n(T,A,x)=limpATn+pxq(pm1)0.

    In this section, we study the product and power of an n-quasi-A-(m,q)-isometry operators.

    Let n(k) be the (descending Pochhammer) symbol defined by:

    n(k)={0if n=0,0if n>0 and k>n,k!(nk)if n>0 and kn.

    Proposition 3.1. T is a n-quasi-A-(m,q)-isometry if and only if we have

    ATn+px=m1j=0(1)mj1p(p1)(pj)(pm+1)j!(mj1)!ATj+nxq,

    for all p0 and all xX, where (pj) denotes that the factor (pj) is omitted.

    Proof. T is a n-quasi-A-(m,q)-isometry if and only if

    ATn+pxq=m1k=0(pk)Qqk,n(T,A,x)=m1k=0(pk)kj=0(1)kj(kj)ATn+jxq=m1j=0ATn+jxqm1k=j(1)kj(pk)(kj).

    By [12, Lemma 2.3], we have

    m1k=j(1)kj(pk)(kj)=(1)mj1p(p1)(pj)(pm+1)j!(mj1)!.

    Then,

    ATn+px=m1j=0(1)mj1p(p1)(pj)(pm+1)j!(mj1)!ATj+nxq.

    Lemma 3.1. Let T be a n-quasi-A-(m,q)-isometry and >m1. For all t{0,,2}, we have

    m+1j=0(1)m+1j(m+1j)ti=0(ji)ATj+nxq=0.

    Proof. Let t{0,,2}, we have

    (m+1j)ti=0(ji)=(m+1)!j!(m+1j)!j(j1)(jt)=(m+t2)!ti=0(m++i)(jt1)!(m+1j)!=(m+t2jt1)t+1i=1(m+i).

    Then

    m+1j=0(1)m+1j(m+1j)ti=0(ji)ATj+nxq=m+1j=0(1)m+1j(m+t2jt1)t+1i=1(m+i)ATj+nxq=t+1i=1(m+i)(m+1j=t+1(1)m+1j(m+t2jt1)ATj+nxq)=t+1i=1(m+i)(m+t2j=0(1)m+t2j(m+t2j)ATj+n(Tt+1x)q)=0.

    Lemma 3.2. Let T be a n-quasi-A-(m,q)-isometry, p0 and m1. Then, there exists a finite sequence (aj,i)m1i=0 such that

    ATp+nxq=m1k=0(1)m1kk!(mk1)![aj,0+m1i=1aj,ii1t=0(pt)]ATn+kxq,

    for j=0,1,...,1.

    Proof. By using [13], there exists a finite sequence (aj,i)m1i=0 such that

    p(p1)(pj)(pm+1)=aj,0+m1i=1aj,ii1t=0(pt).

    Since T is a n-quasi-A-(m,q)-isometry, then by using Proposition 3.1, we obtain that

    ATn+pxq=m1j=0(1)mj1j!(mj1)![p(p1)(pj)(pm+1)]ATj+nxq=m1j=0(1)mj1j!(mj1)![aj,0+m1i=1aj,ii1t=0(pt)]ATj+nxq.

    Theorem 3.1. Let n1,n2,m,l be positive integers and T,SL(X). If T is a n1-quasi-A-(m,q)-isometry and S is a n2-quasi-A-(l,q)-isometry such that ST=TS, then TS is a n-quasi-A-(m+l1,q)-isometry, with n=max(n1,n2).

    Proof. We have

    Qqm+l1,n(TS,A,x)=m+l1k=0(1)m+l1k(m+l1k)A(TS)n+kxq=m+l1k=0(1)m+l1k(m+l1k)ATn+k(Sn+kx)q.

    Using Lemma 3.2, we see that

    Qqm+l1,n(TS,A,x)=m+l1k=0(1)m+l1k(m+l1k)m1j=0(1)mj1j!(mj1)!×[aj,0+m1i=1aj,ii1t=0(pt)]ATn+j(Sn+kx)q=m1j=0(1)mj1j!(mj1)!m+l1k=0(1)m+l1k(m+l1k)[aj,0+m1i=1aj,ii1t=0(pt)]×ATn+j(Sn+kx)q=m1j=0(1)mj1j!(mj1)!aj,0m+l1k=0(1)m+l1k(m+l1k)ASn+k(Tn+jx)q+m1j=0(1)mj1j!(mj1)!m1i=1aj,im+l1k=0(1)m+l1k(m+l1k)×i1t=0(pt)ASn+k(Tn+jx)q.

    Since S is a n2-quasi-A-(l,q)-isometry, then according to Proposition 2.4, we get that S is a n-quasi-A-(m+l1,q)-isometry. Hence,

    m1j=0(1)mj1j!(mj1)!aj,0m+l1k=0(1)m+l1k(m+l1k)ASn+k(Tn+jx)q=0=0.

    Since i=1,...,m1, then, by using Lemma 3.1, we infer that

    m+l1k=0(1)m+l1k(m+l1k)i1t=0(pt)ASn+k(Tn+jx)q=0.

    Consequently, one obtains that

    m1j=0(1)mj1j!(mj1)!m1i=1aj,im+l1k=0(1)m+l1k(m+l1k)i1t=0(pt)ASn+k(Tn+jx)q=0=0,

    which gives that

    Qqm+l1,n(TS,A,x)=0.

    The following example shows that Theorem 3.1 is not necessarily true if S and T are not commuting.

    Example 3.1. We consider the operators on the two dimensional (R2,.2).

    T=(1101),  S=(1011) and A=(1112).

    Note that STTS. Moreover, by a direct computation, we show that T and S are quasi-A-(3,2)-isometry. However neither TS nor ST is a quasi-A-(5,2)-isometry.

    Corollary 3.1. Let n1,n2,m,l be positive integers and T,S,A1,A2L(X) such that TS=ST,A1A2=A2A1,TA1=A1T and SA2=A2S. If T is a n1-quasi-A1-(m,q)-isometry and S is a n2-quasi-A2-(l,q)-isometry, then TS is a n-quasi-A1A2-(m+l1,q)-isometry, with n=max(n1,n2).

    Proof. Following the same steps as in the proof of Theorem 3.1, we can prove that

    Qqm+l1,n(TS,A1A2,x)=0.

    Indeed, we have

    Qqm+l1,n(TS,A1A2,x)=m+l1k=0(1)m+l1k(m+l1k)A1A2(TS)n+kxq=m+l1k=0(1)m+l1k(m+l1k)A1Tn+k(A2Sn+kx)q.

    Theorem 3.2. Let T be a n-quasi-A-(m,q)-isometry. Then, for each positive integer k, Tk is a n-quasi-A-(m,q)-isometry.

    Proof.

    Qqm,n(Tk,A,x)=mj=0(1)mj(mj)A(Tk)n+jxq=mj=0(1)mj(mj)ATkn+kjxq=mj=0(1)mj(mj)m1i=0(kji)Qqi,kn(T,A,x)=m1i=01i![mj=0(1)mj(mj)(kj)(i)]Qqi,kn(T,A,x).

    According to [14, Lemma 1], we have mj=0(1)mj(mj)(kj)(i)=0 for each i=0,1,...,m1. It follows that Qqm,n(Tk,A,x)=0.

    The converse of Theorem 3.2 is not true in general as shown in the following example.

    Example 3.2. Let A=(101011110). It is not difficult to prove that the operator T=(011001000) defined in (R3,.2) satisfies T3 is a quasi-A-(3,2)-isometry but T is not a quasi-A-(3,2)-isometry.

    Proposition 3.2. Let TL(X) and n1,n2,r,s,m,l be positive integers. If Tr is a n1-quasi-A-(m,q)-isometry and Ts is a n2-quasi-A-(l,q)-isometry, then Tt is a n0-quasi-A-(p,q)-isometry, where t is the greatest common divisor of r and s, n0=max(n1,n2) and p=min(m, l).

    Proof. Let's put aj=ATn+jxq,j0. Since Tr is a n1-quasi-A-(m,q)-isometry and Ts is a n2-quasi-A-(l,q)-isometry, then Tr is a n0-quasi-A-(m,q)-isometry and Ts is a n0-quasi-A-(l,q)-isometry. Hence,

    mj=0(1)mj(mj)aj+n0r=0andlj=0(1)lj(lj)aj+n0s=0.

    By [15, Lemma 3.15], we infer that

    pj=0(1)pj(pj)aj+n0t=0,

    which ends the proof.

    As an immediate consequence of Proposition 3.2, we have the following result.

    Corollary 3.2. Let T,AL(X) and r,s,m,n,l be positive integers. Then, the following properties hold.

    (1) If T is a n-quasi-A-(m,q)-isometry such that Ts is a n-quasi-A-(1,q)-isometry, then T is a n-quasi-A-(1,q)-isometry.

    (2) If Tr and Tr+1 are a n-quasi-A-(m,q)-isometries, then T is a n-quasi-A-(m,q)-isometry.

    (3) If Tr is a n-quasi-A-(m,q)-isometry and Tr+1 is a n-quasi-A-(l,q)-isometry with m<l, then T is a n-quasi-A-(m,q)-isometry.

    As an immediate consequence of Proposition 3.2, Theorem 3.1 and Corollary 3.1, we have the following result.

    Corollary 3.3. Let n1,n2,r,s,m,l be positive integers and T,S,A,A1,A2L(X). Let n=max(n1,n2). The following properties hold true.

    (1) If T is a n1-quasi-A-(m,q)-isometry and S is a n2-quasi-A-(l,q)-isometry such that ST=TS, then TrSs is a n-quasi-A-(m+l1,q)-isometry.

    (2) If T is a n1-quasi-A1-(m,q)-isometry and S is a n2-quasi-A2-(l,q)-isometry such that TS=ST, A1A2=A2A1, TA1=A1T and SA2=A2S, then TrSs is a n-quasi-A1A2-(m+l1,q)-isometry.

    We focus on some properties of a new class of operators called n-quasi-A-(m,q)-isometry operators. First, we give spectral properties and relationship between n-quasi-A-(m,q)-isometry and p-quasi-A-(m,q)-isometry. Second, the power and product of such operators have been investigated. As a future work, we can generalize our study on a metric, dislocated metric or dislocated quasi metric space (see references [8,16,17]).

    The authors declare that they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This work is supported by Researchers Supporting Project number (RSPD2023R736), King Saud University, Riyadh, Saudi Arabia.

    The authors declare that there is no conflict of interest



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