Research article Special Issues

Some results on frames by pre-frame operators in Q-Hilbert spaces

  • Quaternionic Hilbert (Q-Hilbert) spaces are frequently used in applied physical sciences and especially in quantum physics. In order to solve some problems of many nonlinear physical systems, the frame theory of Q-Hilbert spaces was studied. Frames in Q-Hilbert spaces not only retain the frame properties, but also have some advantages, such as a simple structure for approximation. In this paper, we first characterized Hilbert (orthonormal) bases, frames, dual frames and Riesz bases, and obtained the accurate expressions of all dual frames of a given frame by taking advantage of pre-frame operators. Second, we discussed the constructions of frames with the help of the pre-frame operators and gained some more general methods to construct new frames. Moreover, we obtained a necessary and sufficient condition for the finite sum of frames to be a (tight) frame, and the obtained results further enriched and improved the frame theory of the Q-Hilbert space.

    Citation: Yan Ling Fu, Wei Zhang. Some results on frames by pre-frame operators in Q-Hilbert spaces[J]. AIMS Mathematics, 2023, 8(12): 28878-28896. doi: 10.3934/math.20231480

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  • Quaternionic Hilbert (Q-Hilbert) spaces are frequently used in applied physical sciences and especially in quantum physics. In order to solve some problems of many nonlinear physical systems, the frame theory of Q-Hilbert spaces was studied. Frames in Q-Hilbert spaces not only retain the frame properties, but also have some advantages, such as a simple structure for approximation. In this paper, we first characterized Hilbert (orthonormal) bases, frames, dual frames and Riesz bases, and obtained the accurate expressions of all dual frames of a given frame by taking advantage of pre-frame operators. Second, we discussed the constructions of frames with the help of the pre-frame operators and gained some more general methods to construct new frames. Moreover, we obtained a necessary and sufficient condition for the finite sum of frames to be a (tight) frame, and the obtained results further enriched and improved the frame theory of the Q-Hilbert space.



    The concept of frames, which generalizes that of bases, was first introduced in the 1950s when Duffin and Schaeffer [1] studied some ongoing problems in the nonharmonic Fourier series. Looking back upon the a sequence {ej:jJ}H (Hilbert space), we call {ej:jJ} is a frame for H if the following inequality holds,

    Ax2jJ|x,ej|2Bx2,xH,

    where positive constants A,B are called the frame bounds. Frames have turned into a hot issue even since 1986 when Daubechies, Crossman and Meyer published their pioneering work [2]. Nowadays, great achievements have been made in the research of frame theory [3,4], and frames have been heavily used in numerous fields, such as coding and wireless communication [5], image and signal processing [6], sampling theory [7], quantum measurements [8], and so on ([9,10]).

    Hilbert space can be defined not only in real field and complex field, but also in quaternion field [11,12]. In 1936, Birkhoff and von Neumann [13] in their famous pioneering work on quantum logic commented that quantum mechanics can also be formulated in Hilbert space where the ground field of complex numbers is replaced by divisible algebras of quaternions [14]. By now, this opinion has been confirmed in the reference [15]. However, it is worth noting that most existing works on the frame theory only focus on real or complex Hilbert spaces instead of quaternionic Hilbert (Q-Hilbert) spaces. Note that both the real field and the complex field are associative and commutative, while the quaternion field only constitutes noncommutative associative algebra. This key characteristic greatly limited mathematicians to establish a complete theory of functional analysis in Q-Hilbert spaces [16], which affected the development of quantum physics in Q-Hilbert space. Luckily, the study on quaternion field has been developed from the mathematical point of view, and achievements in the frames in Q-Hilbert space especially have been obtained in recent. For example, Khokulan, Thirulogasanthar, Srisatkunarajah [17] and Sharma, Virender [18] introduced and studied frames for finite dimensional Q-Hilbert spaces, Sharma, Goel [19] and Sharma, Singh, Sahu [20] studied frames and dual frames for separable Q-Hilbert spaces, and Ellouz [21] introduced K-Frames and Zhang, Li [22] characterized Riesz bases in Q-Hilbert spaces.

    When characterizing dual frames of a frame, constructing new frames is a big issues in frame theory. Finding suitable frames are of great significance in applications, and plenty of achievements have been acquired with regard to such issues. For instance, in [7] Li proved that for a given frame, one could obtain all its dual frames by seeking the left inverse of the invertible operator and then giving the accurate expression of all dual frames of the given frame. In [23], Guo looked to ways of constructing (Ω, μ)-frames, consisting of the structures of new (Ω, μ)-frames and the dual (Ω, μ)-frames in some conditions. In [24], Obeidat, Samarah, Casazza and Tremain went into the sums of frames in Hilbert spaces, and gave simple necessary and sufficient conditions on Bessel sequences {xi}iI and {yi}iI as well as the operators Q1,Q2 on H so that {Q1xi+Q2yi}iI formed a new frame for H. In [25,26]], the authors discussed the sums of g-frames in Hilbert spaces, it was a simple and effective method to construct new frames by using the sums of known frames. Inspired by these works on frames, and aided by the pre-frame operators, we discuss analogous problems on frames in Q-Hilbert spaces. Especially, we obtain some more general construction methods by means of pre-frame operators (see Theorems 3.2 and 4.2), and other current methods. Usually, a new frame can be constructed by using the frame operator and the synthesis (analysis) operator to satisfy certain conditions, such as in [24] where {xj}jJ and {yj}jJ are frames for H with analysis operators T1,T2 and frame operators S1,S2, respectively. {xj+yj}jJ is a new frame for H if and only if S1+S2+T1T2+T2T1>0. Comparatively, the methods we use are more convenient and direct.

    In section two, we give some essential notions and existing results for later use. In section there, we first introduce the notion of the pre-frame operator, which is an important class of operators in frame theory, and characterize orthonormal bases, frames, dual frames and Riesz bases in terms of pre-frame operators. We then we obtain the accurate expressions of all dual frames of a given frame by taking advantage of pre-frame operators. With the help of an operator equation, we also give the characterization of the dual frames in Q-Hilbert spaces. In section four, we discuss the sum of frames and Bessel sequences. By means of pre-frame operators, we gain some more general methods to construct new frames. Moreover, we obtain a necessary and sufficient condition for the finite sum of frames to be a (tight) frame.

    In this section we arrange some notions and results of frames in Q-Hilbert spaces (see [19,20] for details), which are necessary for below. Q denotes a noncommutative quaternion field, and J is an index set. Let HR(Q),KR(Q) be right Q-Hilbert spaces (or simply R-Q-Hilbert spaces) and B(HR(Q),KR(Q)) denote the collection of all bounded right Q-linear operators from HR(Q) to KR(Q), as a special case, HR(Q)=KR(Q), B(HR(Q),KR(Q))=B(HR(Q)), and IHR be the identity operator in HR(Q). For KB(HR(Q)), the range of K is represented by R(K), and the pseudo-inverse of K is represented by K if R(K) is closed.

    The noncommutative field of quaternions Q is a four-dimensional real algebra with unity. In Q, zero denotes the null element and one denotes the identity with respect to multiplication. It also includes three so-called imaginary units, denoted by i,j,k, i.e.,

    Q={x0+x1i+x2j+x3k:x0,x1,x2,x3R},

    where i2=j2=k2=1,ij=ji=k,jk=kj=i and ik=ki=j. For more information about the properties of quaternions, we refer the readers to [11–16].

    Let HR(Q) be a linear vector space under right scalar multiplication over the field of quaternions Q. HR(Q) is called a right quaternionic pre-Hilbert space or right quaternionic inner product space if it is equipped with a Hermitian quaternionic inner product (or simply the inner product)

    |:HR(Q)×HR(Q)Q

    satisfying the following conditions:

    (a)¯ϕ|ψ=ψ|ϕ for all ϕ,ψHR(Q);

    (b)ϕ|ϕ>0 unless ϕ=0;

    (c)ϕ|ψ+ω=ϕ|ψ+ϕ|ω for all ϕ,ψ,ωHR(Q);

    (d)ϕ|ψq=ϕ|ψq, ϕq|ψ=ˉqϕ|ψ for all ϕ,ψHR(Q) and qQ.

    Let HR(Q) be a right quaternionic pre-Hilbert space with the inner product |. We define the quaternionic norm :HR(Q)R+ on HR(Q) by ϕ=ϕ|ϕ,ϕHR(Q). If HR(Q) is complete with respect to the norm , it is called an R-Q-Hilbert space and is denoted by HR(Q).

    Proposition 2.1. ([12]) Let HR(Q) be an R-Q-Hilbert space and NHR(Q) meet that for z,zN zz={1 if z=z;0 if zz. Then the following assertions are equivalent:

    (ⅰ) x,yHR(Q), the progression zNx|zz|y is absolute convergence in HR(Q) and it possess:

    x|y=zNx|zz|y.

    (ⅱ) x=zN|z|x|2, xHR(Q).

    (ⅲ) N={uHR(Q):u|z=0,zN}={0}.

    (ⅳ) spanN is dense in HR(Q).

    Definition 2.1. ([12]) Let HR(Q) be an R-Q-Hilbert space, and NHR(Q) is called a Hilbert basis or orthonormal basis of HR(Q) if it satisfies zz={1 if z=z;0 if zz. for z,zN and all the conditions in Proposition 2.1. What is more, if N is a Hilbert basis of HR(Q), then arbitrary xHR(Q), the decomposition x=zNzz|x is unique and the progression zNzz|x is an absolute convergence in HR(Q).

    Compared with complex Hilbert spaces, Q-Hilbert spaces inherit a great deal of standard properties (see [12,16]).

    Definition 2.2. ([11]) An operator T:HR(Q)HR(Q), for arbitrary ϕ,ψHR(Q) and α,βQ, if T(ϕα+ψβ)=T(ϕ)α+T(ψ)β, then T is called right Q-linear; if there is a constant M>0 such that TϕMϕ, then T is bounded.

    Proposition 2.2. ([12]) Let TB(HR(Q)), and satisfy T=T, then the norm of T is defined as follows

    Top=supfHR(Q),x=1|Tx|x|.

    Proposition 2.3. ([12]) Let HR(Q) be an R-Q-Hilbert space, U,VB(HR(Q)). Then

    (ⅰ) U+V and UVB(HR(Q)). In addition,

    U+VopUop+VopandUVopUopVop;

    (ⅱ) (U+V)=U+V;

    (ⅲ) (UV)=VU,(U)=U;

    (ⅳ) if the operator U is invertible, then (U1)=(U)1;

    (ⅴ) IHR=IHR, where IHR is the identity operator in HR(Q).

    For more background information on Q-Hilbert spaces, see [11,12].

    In [19], Sharma and Goel extended the concept of frame in Hilbert space to the Q-Hilbert space, as described next.

    Definition 2.3. ([19]) Let HR(Q) be an R-Q-Hilbert space. A sequence {xj}jJHR(Q) is called a frame for HR(Q) if there are two finite constants with 0<AB< such that

    Af2jJ|xj|f|2Bf2,fHR(Q). (2.1)

    The numbers A,B are called frame bounds of {xj}jJ. We call {xj}jJ a Bessel sequence for HR(Q) if only the righthand inequality of (2.1) is established in these circumstances, B is called Bessel bound. We call {xj}jJ a λ-tight frame for HR(Q) if A=B=λ. What is more, we call {xj}jJ a Parseval frame for HR(Q) if λ=1.

    Now define the space l2(Q) by

    l2(Q):={{qj}jJ:{qj}jJQsuch thatjJ|qj|2<+},

    and endow l2(Q) with the inner product

    p|q=jJ¯pjqj,p={pj}jJandq={qj}jJl2(Q).

    Then l2(Q) is an R-Q-Hilbert space.

    If {xj}jJ is a frame for HR(Q), then the operator S:HR(Q)HR(Q) defined by

    Sf=jJxjxj|f,fHR(Q),

    and S is called the (right) frame operator related to {fj}jJ. It is understood that S is a right linear bounded invertible operator (see [19]).

    Definition 2.4. ([20]) Let {xj}jJ be a frame for HR(Q). A sequence {yj}jJHR(Q) fulfills

    f=jJxjyj|f=jJyjxj|f,fHR(Q).

    Then {yj}jJ is commonly known as the alternate dual for {xj}jJ in HR(Q).

    Definition 2.5. ([22]) Let HR(Q) be an R-Q-Hilbert space and {xj}jJHR(Q). {xj}jJ has been described as a Riesz basis for HR(Q) if the following conditions are met

    (ⅰ) {xj}jJ is complete, that is, for fHR(Q), if xj|f=0,jJ, then f=0.

    (ⅱ) There are two positive finite constants A and B such that

    AjJ1|qj|2jJ1xjqj2l2(Q)BjJ1|qj|2, (2.2)

    where qjQ,jJ1, J1 is any finite subset of J. A and B are called Riesz bounds of {xj}jJ.

    In this section, we introduce the definition of the pre-frame operators, and utilize the pre-frame operators for characterizing frames and dual frames in the R-Q-Hilbert space HR(Q). For a given frame in HR(Q), we also obtain the accurate expression formula about the dual frames. For these purposes, we first introduce a lemma, which was given by Sharma and Goel in [19].

    Lemma 3.1. ([19]) Let HR(Q) be an R-Q-Hilbert space and {xj}jJHR(Q). Then {fj}jJ is a Bessel sequence for HR(Q) with bound B if and only if the right linear operator T:l2(Q)HR(Q) defined by

    T({qj}jJ)=jJxjqj,{qj}jJl2(Q),

    is well defined, and TopB.

    Proposition 3.1. Let HR(Q) be an R-Q-Hilbert space and N={zj}jJ be a Hilbert basis for HR(Q). Then {xj}jJHR(Q) is a Bessel sequence for HR(Q) if and only if there exists a unique bounded right linear operator V:HR(Q)HR(Q) such that xj=Vzj for all jJ.

    Proof. (). Note that N={zj}jJ is a Hilbert basis for HR(Q), and therefore {zj|f}jJl2(Q) for each fHR(Q). If {xj}jJHR(Q) is a Bessel sequence, then the operator

    V:HR(Q)HR(Q),Vf=jJxjzj|f,fHR(Q)

    is well defined by Lemma 3.1. We obtain for each fHR(Q) that

    Vf=supgHR(Q),g=1|jJxjzj|f|g|=supgHR(Q),g=1|jJ¯zj|fxj|g|=supgHR(Q),g=1|jJf|zjxj|g|supgHR(Q),g=1(jJ|zj|f|2)12(jJ|xj|g|2)12Bf,

    where B is Bessel bound of {xj}jJ. It follows that V is a bounded right linear operator on HR(Q). By the definition of Hilbert basis, for an arbitrary fHR(Q), we obtain that f=jJzjqj, where {qj}jJl2(Q) is unique, and

    Vf=V(jJzjqj)=jJxjzj|iJziqi=jJxjiJzj|ziqi=jJxjqj.

    Hence jJVzjqj=jJfjqj, which implies that xj=Vzj. Suppose that V1,V2B(HR(Q)) and V1zj=V2zj=xj for all jJ. For fHR(Q), we have (V1V2)zj|f=0 for all jJ. It follows that

    0=jJ|(V1V2)zj|f|2=jJ|zj|(V1V2)f|2=(V1V2)f2,

    and thus V1=V2. Hence the operator V is unique.

    (). If VB(HR(Q)) satisfies xj=Vzj for arbitrary jJ, then

    jJ|xj|f|2=jJ|Vzj|f|2=jJ|zj|Vf|2=Vf2V2opf2,fHR(Q).

    This shows that {xj}jJ is a Bessel sequence for HR(Q).

    Definition 3.1. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q) and {xj}jJ be a Bessel sequence in HR(Q). The operator V in Proposition 3.1 is called the (right) pre-frame operator associated with {xj}jJ.

    Lemma 3.2. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q) and {xj}jJ be a Bessel sequence in HR(Q). If V is the pre-frame operator associated with {xj}jJ and S is the frame operator associated with {xj}jJ, then S=VV.

    Proof. By the definition of V, xj=Vzj for jJ, then

    Sf=jJfjxj|f=jJVzjVzj|f=jJVzjzj|Vf=V(jJzjzj|Vf)=VVf

    for fHR(Q). Hence S=VV.

    Now, we characterize frames and dual frames in terms of pre-frame operators. We begin with a lemma.

    Lemma 3.3. ([21]) Let HR(Q),KR(Q) be two R-Q-Hilbert spaces, and K:HR(Q)KR(Q) be a bounded operator. If R(K) is closed, then, there is a bounded operator K:KR(Q)HR(Q) for which

    KKf=f,fR(K).

    Theorem 3.1. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q) and {xj}jJ be a Bessel sequence for HR(Q). If V and S denote the pre-frame operator and frame operator of {xj}jJ, respectively, then

    (i) {xj}jJ is a frame for HR(Q) if and only if V is onto.

    (ii) {xj}jJ is a Parseval frame for HR(Q) if and only if V is coisometry (i.e., V is isometry).

    (iii) {xj}jJ is a Riesz basis for HR(Q) if and only if V is invertible.

    (iv) {xj}jJ is a Hilbert basis for HR(Q) if and only if V is unitary.

    Proof. (ⅰ) If {xj}jJ is a frame for HR(Q), then S is invertible by (Theorem 3.5 in [19]). By Lemma 3.2, we have S=VV, so V is onto. On the other hand, if V is onto, then {xj}jJ is a Bessel sequence for HR(Q) by Lemma 3.1. Next we only need to show the existence of lower frame bound. Note that V is onto, we have VV=IHR by Lemma 3.3. It follows that (V)V=IHR. Accordingly,

    f2=(V)Vf2(V)2opVf2,fHR(Q).

    Thus,

    jJ|xj|f|2=jJ|Vzj|f|2=jJ|zj|Vf|2=Vf21(V)2opf2.

    (ⅱ) It is easy to check that {xj}jJ is a Parseval frame for HR(Q) iff S is an identity operator on HR(Q). By Lemma 3.2, we have S=VV, so S=IHR if and only if V is a coisometry.

    (ⅲ) See Theorem 3.7 in [22].

    (ⅳ) If {xj}jJ is a Hilbert basis for HR(Q), then we have for any fHR(Q) that

    f2=jJ|xj|f|2=jJ|Vzj|f|2=jJ|zj|Vf|2=Vf2.

    Therefore, VV=IHR. It follows that V is a unitary operator. On the contrary, if V is a unitary operator, then for any fHR(Q), by simple calculation we have

    jJ|xj|f|2=jJ|Vzj|f|2=jJ|zj|Vf|2=Vf2=f2.
    xi|xj=Vzi|Vzj=VVzi|zj=zi|zj=δij,for eachi,jJ.

    So, {xj}jJ is a Hilbert basis for HR(Q).

    Theorem 3.2. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q). Let {xj}jJ and {yj}jJ be Bessel sequences for HR(Q), and let the pre-frame operators related with {xj}jJ and {yj}jJ be V and W, respectively. Then, {xj}jJ and {yj}jJ are dual frames if and only if VW=IHR or WV=IHR.

    Proof. Note that V and W are pre-frame operators related with {xj}jJ and {yj}jJ, respectively, so we have

    xj=Vzjandyj=Wzj,jJ.

    Hence, for fHR(Q), we have

    jJxjyj|f=jJVzjWzj|f=V(jJzjzj|Wf)=VWf.

    Similarly,

    jJyjxj|f=jJWzjVzj|f=W(jJzjzj|Vf)=WVf.

    It can be seen from this that {xj}jJ and {yj}jJ are dual frames if and only if VW=IHR or WV=IHR.

    If U,VB(HR(Q)) and UV=IHR, then U is called a left inverse operator of V. Our next goal is to characterize dual frames for the existing frame in an R-Q-Hilbert space. The following theorem gave the characterization of the right linear bounded left inverses of the existing pre-frame operator.

    Theorem 3.3. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q) and {xj}jJ be a frame for HR(Q). Suppose that {yj}jJHR(Q) and the pre-frame operator of {xj}jJ is V, then {yj}jJ is a dual frame of {xj}jJ if and only if yj=Wzj for an arbitrary jJ, where W is a right linear bounded left inverse of V.

    Proof. (). Let {yj}jJ be an arbitrary dual frame of {xj}jJ, and W be the pre-frame operator of {yj}jJ. There is a bounded right linear operator W such that yj=Wzj for arbitrary jJ by Proposition 3.1, and so for fHR(Q), we have

    f=jJxjyj|f=jJyjxj|f.

    Note as V as the pre-frame operator of {xj}jJ, we have xj=Vzj for arbitrary jJ, so

    f=jJxjyj|f=jJVzjWzj|f=V(jJzjzj|Wf)=VWf.

    This implies that VW=IHR. Therefore, WV=IHR, as required.

    (). Let yj=Wzj for any jJ, where the bounded right linear operator W is a left inverse of V. Since WV=IHR, WB(HR(Q)) is surjective. Hence {yj}jJ is a frame for HR(Q) by Theorem 3.1 (i). For all fHR(Q), we have

    jJxjyj|f=jJVzjWzj|f=V(jJzjzj|Wf)=VWf=WVf=f.

    Thus, {yj}jJ is an arbitrary dual frame of {xj}jJ by Definition 2.4.

    Theorem 3.3 suggests the operator W has great independent interest. To have a better understanding of W, we prove the following lemma.

    Lemma 3.4. Let {xj}jJ be a frame for an R-Q-Hilbert space HR(Q), and its pre-frame operator and frame operator are V and S, respectively. Then WB(HR(Q)) is a left invertible operator of V if and only if

    W=S1V+U(IHRVS1V),

    where UB(HR(Q)).

    Proof. Suppose that WB(HR(Q)) is an arbitrary left invertible of V. Let U=W, then

    S1V+U(IHVS1V)=S1V+WWVS1V=S1V+WS1V=W.

    Conversely, we suppose that W=S1V+U(IHRVS1V), by Lemma 3.2, and we have

    WV=S1VV+U(IHRVS1V)V=S1S+U(VVS1VV)=IHR+UVUVS1VV=IHR.

    Hence W is a bounded right linear left inverse of V.

    Based on Theorem 3.3 and Lemma 3.4, we characterize all dual frames for an arbitrarily given frame in R-Q-Hilbert spaces, and give the accurate expressions of all dual frames by taking advantage of pre-frame operators.

    Theorem 3.4. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q). If {xj}jJ is a frame for HR(Q), V and S are the pre-frame operator and frame operator of {xj}jJ, respectively, then the sequence {yj}jJHR(Q) is a dual frame for {xj}jJ if and only if

    yj=S1xj+UzjUVS1xj,jJ,

    where UB(HR(Q)) is a right linear operator.

    Proof. (). Suppose that the sequence {yj}jJHR(Q) is an arbitrary dual frame for {xj}jJ. The results in Theorem 3.3 show that yj=Wzj for arbitrary jJ, where W is a left inverse of V. By Lemma 3.4, we have

    W=S1V+U(IHRVS1V)

    for some right linear operator UB(HR(Q)). Hence, for any jJ, we have

    yj=Wzj=(S1V+U(IHVS1V))zj=S1Vzj+U(IHRVS1V)zj=S1xj+UzjUVS1Vzj=S1xj+UzjUVS1xj.

    (). Assume that

    yj=S1xj+UzjUVS1jj,for all jJ.

    where UB(HR(Q)) is a right linear operator. Next to prove that {yj}jJ is an arbitrary dual frame for {xj}jJ, note that V is the pre-frame operator of {xj}jJ, then

    yj=S1xj+UzjUVS1xj=S1Vzj+UzjUVS1Vzj=(S1V+UUVS1V)zj.

    It is easy to prove that {yj}jJ is a Bessel sequence for HR(Q). Let W denote the pre-frame operator of {yj}jJ, then

    W=S1V+UUVS1V=S1V+U(IHVS1V).

    Thus, W is a bounded right linear left inverse of V by Lemma 3.4. We conclude that {yj}jJ is what we are looking for by Theorem 3.3.

    At the end of this section, we give some characterizations of dual frames by taking advantage of operator equations.

    Theorem 3.5. Let {xj}jJ be a Parseval frame for an R-Q-Hilbert space HR(Q), and {yj}jJ be a frame for HR(Q). Use Tx,Ty to denote the pre-frame operators of {xj}jJ and {yj}jJ, respectively. Suppose that Px is the orthogonal projection: l2(Q)R(Tx), then {yj}jJ is a dual frame of {xj}jJ if and only if PxTy=Tx.

    Proof. (). Note that {xj}jJ is a Parseval frame for HR(Q), TxTx=IHR by Lemma 3.2. Hence TxTx=Px. If {yj}jJ is a dual frame of {xj}jJ, then TxTy=IHR. It follows that PxTy=TxTxTy=Tx.

    (). Since Tx=PxTy=TxTxTy, TxTxTxTy=0, i.e., Tx(IHRTxTy)=0. By Theorem 3.12 in [19], we know that Tx is onto, so we have TxTy=IHR. Therefore, {yj}jJ is a dual frame of {xj}jJ.

    Theorem 3.6. Let {xj}jJ and {yj}jJ be frames for an R-Q-Hilbert space HR(Q), and their pre-frame operators be Tx and Ty, respectively. If Px is an orthogonal projection from l2(Q) to R(Tx), then {yj}jJ is a dual frame of {xj}jJ if and only if PxTy=TxS1x, where Sx denotes the frame operator of {xj}jJ.

    Proof. In accordance with Theorem 3.9 in [19], we have {S12xfx}jJ is a Parseval frame for HR(Q) if {xj}jJ is a frame for HR(Q). The rest is similar to the proof of Theorem 3.5.

    In application, constructing new frames is one of the active research directions. In [24], the authors debated the constructions of frames by means of the sum of frames in Hilbert spaces. Inspired by their work, in this section, we will apply the pre-frame operators to discuss the finite sum of frames in R-Q-Hilbert spaces, which generalize the corresponding results on general frames in Hilbert spaces. At first, we give an example.

    Example 4.1. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q). Define two sequences {xj}jJ,{yj}jJHR(Q) by

    {x1=z1,xj=zj1,forj2,jJ,

    and yj=xj for all jJ. Through simple calculation, we know that {xj}jJ and {yj}jJ are frames for HR(Q), but {xj+yj}jJ is not frame for HR(Q). Define xj=zj for every jJ and yj=1jzj for every jJ, then {xj+yj}jJ is frame for HR(Q). However, {yj}jJ is not a frame but a Bessel sequence for HR(Q).

    By Example 4.1, it shows that the sum of frames for HR(Q) is not a new frame. It is natural to ask for some proper conditions, and when the conditions have been established, the sum of frames is a frame in R-Q-Hilbert spaces. The following theorems give some sufficient conditions on the frame {xj}jJ and Bessel sequence {yj}jJ, which lead to new frames of the form {αxj+βyj}jJ or {αjxj+βjyj}jJ.

    Theorem 4.1. Suppose that {xj}jJ is a frame for an R-Q-Hilbert space HR(Q), and its frame bounds are A and B; {yj}jJ is a Bessel sequence for HR(Q) and its Bessel bound is B1. If A,B and B1 satisfy

    A|α|22B1|β|2>0

    for non-zero constants α,βQ, then a new frame of the form {αxj+βyj}jJ can be constructed for HR(Q).

    Proof. To prove that {αxj+βyj}jJ is a newly constructed frame for HR(Q), we must find the upper and lower bounds of {αxj+βyj}jJ. For fHR(Q), we have

    jJ|(αxj+βyj)|f|2jJ(|αxj|f|+|βyj|f|)2=jJ|αxj|f|2+jJ|βyj|f|2+2jJ|αxj|f||βyj|f|jJ|αxj|f|2+jJ|βyj|f|2+2(jJ|αxj|f|2)12(jJ|βyj|f|2)122jJ|αxj|f|2+2jJ|βyj|f|2=2|α|2jJ|xj|f|2+2|β|2jJ|yj|f|22(|α|2B+|β|2B1)f2.

    Similarly,

    jJ|αxj|f|2=jJ|(αxj+βyj)|fβyj|f|22jJ|(αxj+βyj)|f|2+2jJ|βyj|f|2,

    and it follows that

    2jJ|(αxj+βyj)|f|2jJ|αxj|f|22jJ|βyj|f|2=|α|2jJ|xj|f|22|β|2jJ|yj|f|2(|α|2A2|β|2B1)f2.

    Thus, we have

    12(|α|2A2|β|2B1)f2jJ|(αxj+βyj)|f|22(|α|2B+|β|2B1)f2.

    Observe that A|α|22B1|β|2>0, then {αxj+βyj}jJ is a newly constructed frame for HR(Q).

    Theorem 4.2. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q). Suppose that {xj}jJ is a frame for HR(Q), and its frame bounds are A and B; {yj}jJ is a Bessel sequence for HR(Q) and its pre-frame operator is V. For any two families {αj}jJ and {βj}jJ (αj,βjQ,jJ), if

    V2<AinfjJ|αj|22supjJ|βj|2,

    then {αjxj+βjyj}jJ is a newly constructed frame for HR(Q).

    Proof. For all fHR(Q), we have

    jJ|(αxj+βyj)|f|22(jJ|αxj|f|2+jJ|βyj|f|2)2((supjJ|αj|2)jJ|xj|f|2+(supjJ|βj|2)jJ|yj|f|2)=2((supjJ|αj|2)jJ|xj|f|2+(supjJ|βj|2)jJ|Vzj|f|2)2((supjJ|αj|2)Bf2+(supjJ|βj|2)Vf2)2((supjJ|αj|2)B+(supjJ|βj|2)V2)f2.

    On the other hand, since

    jJ|αxj|f|2=jJ|(αxj+βyj)|fβyj|f|22jJ|(αxj+βyj)|f|2+2jJ|βyj|f|2,

    then,

    2jJ|(αxj+βyj)|f|2jJ|αxj|f|22jJ|βyj|f|2(infjJ|αj|2)jJ|xj|f|22(supjJ|βj|2)jJ|Vzj|f|2=(infjJ|αj|2)jJ|xj|f|22(supjJ|βj|2)Vf2(A(infjJ|αj|2)2(supjJ|βj|2)V2)f2.

    If V2<AinfjJ|αj|22supjJ|βj|2, then A(infjJ|αj|2)2(supjJ|βj|2)V2>0, so {αjxj+βjyj}jJ is a newly constructed frame for HR(Q).

    From Theorem 4.2, we have the following corollary.

    Corollary 4.1. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q). Suppose that {xj}jJ is a frame for HR(Q), and its frame bounds are A and B; {yj}jJ is a Bessel sequence for HR(Q) with the pre-frame operator V. If V2<A2, then {xj+yj}jJ is a new frame for HR(Q).

    Theorem 4.3. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q). Assume that {xj}jJ and {yj}jJ are both frames for HR(Q), and Vx, Vy are their pre-frame operators, respectively. If the condition VyVx=0 is met, then {xj+yj}jJ is a newly constructed frame for HR(Q). Moreover, if {xj}jJ and {yj}jJ are both one-tight frames for HR(Q) and VyVx=0, then {xj+yj}jJ is a two-tight frame for HR(Q).

    Proof. Note that the pre-frame operators of {xj}jJ and {yj}jJ are Vx and Vy, respectively. It can be seen from their definitions

    xj=Vfzjandyj=Vgzj,for alljJ.

    Hence xj+yj=Vxzj+Vyzj=(Vx+Vy)zj for any jJ. To show {xj+yj}jJ is a frame for HR(Q), it is sufficient to show Vx+Vy is onto by Theorem 3.1. Using VyVx=0, we have

    (Vx+Vy)Vx=VxVx+VyVx=VxVx.

    Once again, to utilize the invertibility of VxVx, for an arbitrary element g in HR(Q), taking f=Vx(VxVx)1g, undoubtedly, fHR(Q) satisfies

    (Vx+Vy)f=(Vx+Vy)Vx(VxVx)1g=(VxVx)(VxVx)1g=g.

    Thus Vx+Vy is onto.

    Especially, if {xj}jJ and {yj}jJ are both one-tight frames for HR(Q), and their pre-frame satisfies operators VyVx=0, then {xj+yj}jJ is a frame for HR(Q) by the proof of the previous part. Letting Sx+y denote the frame operator of {xj+yj}jJ, for any fHR(Q), we know that

    Sx+yf=jJ(xj+yj)(xj+yj)|f=jJxjxj|f+jJxjyj|f+jJyjxj|f+jJyjyj|f=VxVxf+jJVxzjVyzj|f+jJVyzjVxzj|f+VyVyf=2f+VxVyf+VyVxf+=2f.

    Thus,

    jJ|(xj+yj)|f|2=Sx+yf|f=2f|f=2f2.

    It follows that {xj+yj}jJ is a two-tight frame for HR(Q).

    Extend the number of frames to a finite number and we have the following corollary.

    Corollary 4.2. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q). Suppose that {x1,j}jJ, {x2,j}jJ,,{xl,j}jJ are frames for HR(Q), and V1,V2,,Vl are pre-frame operators associated with {x1,j}jJ,{x2,j}jJ,,{xl,j}jJ, respectively. If VmVn=0,m,n=1,2,,l, then {x1,j+x2,j++xl,j}jJ is a frame for HR(Q). Moreover, if {x1,j}jJ,{x2,j}jJ,,{xl,j}jJ are one-tight frames for HR(Q) and VmVn=0,m,n=1,2,,l, then {x1,j+x2,j++xl,j}jJ is an l-tight frame for HR(Q).

    More generally, we have the following theorem.

    Theorem 4.4. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q). Assume that {xj}jJ and {yj}jJ are both frames for HR(Q), and Vx, Vy are their pre-frame operators, respectively, and satisfy VyVx=0. If P,QB(HR(Q)), and P or Q is onto, then {Pxj+Qyj}jJ is a frame for HR(Q).

    Proof. Note that the pre-frame operators of {xj}jJ and {yj}jJ are Vx and Vy, respectively. It can be seen from their definitions

    xj=Vxzjandyj=Vyzj,for alljJ.

    After a simple calculation,

    Pxj+Qyj=PVxzj+QVyzj=(PVx+QVy)zj.

    To show {Pxj+Qyj}jJ is a frame for HR(Q), it is sufficient to show that the operator PVx+QVy is onto by Theorem 3.1. By Lemma 3.2, we know that VxVx is invertible. Without loss of generality, let us suppose P is onto. For an arbitrary element gHR(Q), there is always fHR(Q) meets Pf=g. Thus, for any gHR(Q) and taking h=Vx(VxVx)1f, undoubtedly, hHR(Q) satisfies

    (PVx+QVy)h=(PVx+QVy)Vx(VxVx)1f=PVxVx(VxVx)1f+QVyVx(VxVx)1f=PVxVx(VxVx)1f=Pf=g.

    So PVx+QVy is onto.

    In particular, to two one-tight frames in an R-Q-Hilbert space, a necessary and sufficient condition is given, for which the new frame is tight.

    Theorem 4.5. Let N={zj}jJ be a Hilbert basis for an R-Q-Hilbert space HR(Q). Assume that {xj}jJ and {yj}jJ are two one-tight frames for HR(Q), Vx, Vy are their pre-frame operators, respectively, and satisfy VyVx=0. Let U1,U2B(HR(Q)), then {U1xj+U2yj}jJ is a λ-tight frame for HR(Q) if and only if U1U1+U2U2=λIHR.

    Proof. Note that Vx and Vy are pre-frame operators associated with {xj}jJ and {yj}jJ, respectively. For every jJ, we have

    xj=Vxzjandyj=Vyzj.

    For any fHR(Q), we have

    jJ|(U1xj+U2yj)|f|2=jJf|(U1xj+U2yj)(U1xj+U2yj)|f=jJ(f|U1xj+f|U2yj)(U1xj|f+U2yj|f)=jJ|U1xj|f|2+jJf|U1xjU2yj|f+jJf|U2yjU1xj|f+jJ|U2yj|f|2=jJ|xj|U1f|2+jJU1f|xjyj|U2f+jJU2f|yjxj|U1f+jJ|yj|U2f|2=U1f2+U2f2+jJVxU1f|zjzj|VyU2f+jJVyU2f|zjzj|VxU1f=U1f2+U2f2+VxU1f|VyU2f+VyU2f|VxU1f=U1f2+U2f2+VyVfU1f|U2f+U2f|VyVxU1f=U1f2+U2f2=(U1U1+U2U2)f|f.

    It follows that {U1xj+U2yj}jJ is a λ-tight frame for HR(Q) if and only if U1U1+U2U2=λIHR.

    In the end, a necessary and sufficient condition is given, for which the finite sum of frames to be a frame in an R-Q-Hilbert space.

    Theorem 4.6. Let {x1,j}jJ, {x2,j}jJ,,{xl,j}jJ be frames for an R-Q-Hilbert space HR(Q), and Ai and Bi be the lower and upper bounds of the frame {xi,J}jJ for each i{1,2,,l}, respectively. Let {α1,α2,,αl} (αiQ,i=1,2,,l) be any given scalars, then {li=1αixi,j}jJ is a frame for HR(Q) if and only if there exists an M>0 and some p{1,2,,l} such that

    MjJ|xp,j|f|2jJ|li=1αixi,j|f|2,fHR(Q).

    Proof. (). Note that {xi,j}jJ(i=1,2,,l) is a frame for HR(Q) with frame bounds Ai and Bi. We have for some p{1,2,,l} that

    Apf2jJ|xp,j|f|2Bpf2,fHR(Q).

    It follows that

    1BpjJ|xp,j|f|2f2,fHR(Q).

    Assume that {li=1αixi,j}jJ is a frame for HR(Q) with the lower and upper bounds A and B, respectively. We have for each fHR(Q) that

    Af2jJ|li=1αixi,j|f|2Bf2,

    so

    f21AjJ|li=1αixi,j|f|2,

    for fHR(Q). Therefore, we can conclude that

    ABpjJ|xp,j|f|2jJ|li=1αixi,j|f|2,

    for fHR(Q). Taking M=ABp>0, we have for any fHR(Q) that

    MjJ|xp,j|f|2jJ|li=1αixi,j|f|2.

    (). For each i{1,2,,l}, let M>0 be a constant such that for some p{1,2,,l},

    MjJ|xp,j|f|2jJ|li=1αixi,j|f|2,fHR(Q).

    Since {xi,j}jJ(i=1,2,,l) is a frame, we have

    Apf2jJ|xp,j|f|2Bpf2,fHR(Q),

    so

    MApf2MjJ|xp,j|f|2jJ|li=1αixi,j|f|2,fHR(Q),

    and the lower bound of {li=1αixi,j}jJ exists. Next, we look for the upper bound of {li=1αixi,j}jJ, we will show that {li=1aixi,j}jJ is a Bessel sequence for HR(Q), we have for all fHR(Q) that

    jJ|li=1αixi,j|f|2jJl(li=1|αixi,j|f|2)=lli=1(|αi|2jJ|xi,j|f|2)=l(max1il{|αi|2})(li=1Bi)f2l2max1il{|αi|2}max1il{Bi}f2.

    Therefore, {li=1aixi,j}jJ is a frame for HR(Q).

    Frames in Q-Hilbert spaces both retain the frame properties, and also have some advantages, such as simple structure for approximation. In this paper, the definition of pre-frame operator was introduced. We characterized the Hilbert (orthonormal) bases, frames, dual frames and Riesz bases, and obtained the accurate expressions of all dual frames of a given frame by taking advantage of pre-frame operators. We also discussed the constructions of frames with the help of the pre-frame operators, and gained some more general methods to construct new frames. The obtained results further enriched the frame theory in Q-Hilbert spaces.

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

    The authors would like to express their sincere thanks to the anonymous reviewers for their helpful comments.

    The work was supported the Key Scientific Research Projects of Henan Colleges and Universities (Grant No. 21A110004).

    The authors declare that there are no conflicts of interest.



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