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Research article

g-frame generator sets for projective unitary representations

  • Received: 17 March 2024 Revised: 24 April 2024 Accepted: 08 May 2024 Published: 13 May 2024
  • MSC : 42C15, 42C40, 47D03

  • Frames with special structures play a crucial role in various industrial applications, such as medical imaging, quantum communication, recognition and identification software, and so on. In this paper, we will discuss a more general setting, i.e., a g-frame induced by the projective unitary representation. We show some new results on the dilation property for g-frame generator sets for unitary groups and projective unitary representations. In particular, by using complete wandering operators, several properties of g-frame generators for projective unitary representations have been obtained. Moreover, we explore some characterizations of the g-frame generator dual pairs.

    Citation: Aifang Liu, Jian Wu. g-frame generator sets for projective unitary representations[J]. AIMS Mathematics, 2024, 9(6): 16506-16525. doi: 10.3934/math.2024800

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  • Frames with special structures play a crucial role in various industrial applications, such as medical imaging, quantum communication, recognition and identification software, and so on. In this paper, we will discuss a more general setting, i.e., a g-frame induced by the projective unitary representation. We show some new results on the dilation property for g-frame generator sets for unitary groups and projective unitary representations. In particular, by using complete wandering operators, several properties of g-frame generators for projective unitary representations have been obtained. Moreover, we explore some characterizations of the g-frame generator dual pairs.



    Frames have appeared implicitly in the mathematical literature before they were introduced officially by Duffin and Schaeffer in the context of the non-harmonic Fourier series [1]. Since the celebrated work by Daubechies et al. [2], frame theory has recently become an important tool in many fields such as sampling theory, signal processing and data compression. In recent years, various generalizations of frames have been proposed for different purposes such as frames of subspaces (fusion frames), oblique frames, pseudo-frames, outer frames and g-frames [3,4,5,6,7]. Indeed, all of these generalizations can be regarded as special cases of g-frames [7]. Today, g-frames, with their applications, have been investigated by many researchers [8,9,10,11,12]. As is well known, frames with a special structure, such as Gabor frames and wavelet frames, not only have great variety for use in applications, but also they have undergone extensive theoretical analysis [13,14,15]. Moreover, the dilation property is very important in frame theory and has attracted much attention from scholars from different related fields. The classical dilation theorem for frames shows that every frame for a Hilbert space can be dilated to be a Riesz basis for a larger space [15]. Motivated by these aspects of frames, in this work, we are interested in the dilations of the more general g-frames that are generated by a unitary group, or by a projective unitary representation. In addition, we would like to work more with dual g-frame generators for projective unitary representations.

    Throughout this paper, H and K are two Hilbert spaces over the field of complex numbers and I is the identity operator on H. The notation B(H,K) refers to the space of all bounded linear operators from H into K, and we write B(H)=B(H,H) as the shorthand. Denote by {Hi:iJ} a sequence of subspaces of K and by B(H,Hi) the collection of all bounded linear operators from H into Hi for every iJ, where J is a countable index set. Let {ΛiB(H,Hi)}iJ be a family of operators. If there exist two constants A and B with 0<AB< such that

    A||f||2iJ||Λif||2B||f||2,  fH,

    we call {ΛiB(H,Hi)}iJ a g-frame for H with respect to {Hi}iJ, where A and B are called the lower and upper frame bounds, respectively. For simplification, if the spaces are clear, we will just say that {Λi}iJ is a g-frame for H in the sequel. If we only have the upper bound, then {Λi}iJ is said to be a g-Bessel sequence for H. {Λi}iJ is called a tight g-frame for H if A=B, and a Parseval g-frame for H provided that A=B=1 [7].

    If {Λi}iJ is a g-frame for H, then we can define the operator S:HH by

    Sf=iJΛiΛif,  fH,

    where Λi is the adjoint operator of Λi. Obviously, S is a well-defined, bounded, positive, invertible operator on H. Noted that S is a g-frame operator that is associated with {Λi}iJ. Another fact is that {ΛiS1}iJ is also a g-frame for H and {ΛiS12}iJ is a Parseval g-frame for H (see [7]).

    {ΛiB(H,Hi)}iJ is called a g-orthonormal basis for H if it satisfies the following:

    Λi1fi1,Λi2fi2=δi1,i2fi1,fi2, i1,i2J,fi1Hi1,fi2Hi2,
    iJ||Λif||2=||f||2, fH,

    where δi1,i2 is the Kronecker delta. Actually, by [16, Corollary 2.13], {Λi}iJ is a g-orthonormal basis if and only if {Λi}iJ is a g-frame and the first equation holds.

    The organization of this article is as follows. In Section 2, the dilation results for g-frame generator sets for unitary group will be given. In Section 3, we focus on the g-frame generator sets for projective unitary representation of countable groups and consider the corresponding dilation property. In Section 4, we give some characterizations of g-frame generators for projective unitary representation in terms of complete wandering operators. Moreover, we study some properties of g-frame generators. In Section 5, we introduce the notion of dual g-frame generators and explore some equivalent characterizations of g-frame generator dual pairs.

    In this section, we mainly focus on the dilation problem for g-frame generator sets for a countable unitary group, as well as present some existing dilation results.

    Recall that a unitary system is a subset of unitary operators acting on H which contains the identity operator I in B(H) [17]. Evidently, a unitary group is a special case of unitary system. Two unitary systems U1 and U2 acting on Hilbert spaces H1 and H2, respectively, are said to be unitarily equivalent if there is a unitary operator T:H1H2 such that TU1T=U2.

    According to [18], if H1,H2 are Hilbert spaces, let H1H2 be the algebraic tensor product over C. Denote an inner product on H1H2 by

    ξ1ξ2,η1η2=ξ1,η11ξ2,η22, ξ1,η1H1,ξ2,η2H2

    extended by linearity, where ,i is the inner product of Hi. Then the Hilbert space tensor product H1H2 is the completion of H1H2. Generally, if S1,T1B(H1) and S2,T2B(H2), we can define S1S2B(H1H2) by

    (S1S2)(ξη)=S1ξS2η,  ξH1,ηH2.

    Then (S1S2)(T1T2)=S1T1S2T2,S1(S2+T2)=(S1S2+S1T2) and (S1S2)=S1S2.

    In what follows, we use J to denote a countable index set and IJ to denote a finite set.

    Definition 2.1. ([19, Definition 2.1]) Let U be a countable unitary system on H and {ΛiB(H,K)}iJ. We say that {Λi}iJ is a g-Bessel sequence (g-frame, Parseval g-frame, or tight g-frame) generator set for U if {ΛiU}iJ,UU is a g-Bessel sequence (g-frame, Parseval g-frame, or tight g-frame) for H.

    In particular, for ΛB(H,K), we say that Λ is a g-Bessel sequence (g-frame, Parseval g-frame, or tight g-frame) generator for U if {ΛU}UU is a g-Bessel sequence (g-frame, Parseval g-frame, or tight g-frame) for H.

    Inspired by the above definition, we introduce the following notion.

    Definition 2.2. Let U be a countable unitary system on H and {ΛiVB(H,K)}iJ,VU. {ΛiV}iJ,VU is called a diagonal (Parseval or tight) g-frame generator set for U if {δVUΛiVU}iJ,V,UU is a (Parseval or tight) g-frame for H, where δVU is the Kronecker delta.

    Remark 2.3. Let IJ be a finite set and U be a countable unitary system. For a Hilbert space K, define an operator

    LiU:K2(I×U)K,
    LiUk=eiUk,   kK,

    where {eiU:iI,UU} is the standard basis of 2(I×U) and denotes a tensor product. It is easy to check that, for each a2(I×U) and kK,

    LiU:2(I×U)KK,
    LiU(ak)=a,eiUk.

    We see from Lemma 2.9 in [19] that, for a g-frame generator set {ΛiB(H,K)}iI for U, the analysis operator of {ΛiU}iI,UU is defined by

    θ:H2(I×U)K,
    θf=iI,UULiUΛiUf, fH.

    The operator S:HH given by

    Sf=θθf=iI,UUUΛiΛiUf, fH,

    is called the g-frame operator of {ΛiU}iI,UU. Particularly, if Λ is a g-frame generator for U, the analysis operator of {ΛU}UU can be defined by

    θ:H2(U)K,
    θf=UUeUΛUf,   fH,

    where {eU}UU is the standard basis for 2(U).

    Let U be a unitary group and {eiU:iI,UU} be the standard basis of 2(I×U). For each UU, we define the unitary operator on 2(I×U) by λUeiV=ei(UV), where iI,VU.

    The following result shows that a g-frame generator set for a unitary group is an image of an orthonormal basis under a positive operator with a suitable spectrum.

    Theorem 2.4. Let U be a unitary group on H and {ΛiB(H,K)}iI be a g-frame generator set for U with the frame bounds A and B. Then,

    (1) there exists an isometry Φ:H2(I×U)K such that Φ(λUIK)Φ=U for all UU, where IK is the identity operator on K;

    (2) there exists a positive operator Ξ:2(I×U)KΦ(H) such that {A12,B12}σ(Ξ|Φ(H))[A12,B12] and, for any UU and gK,

    Ξ(eiUg)=ΦUΛig,

    where σ(Ξ|Φ(H)) denotes the spectrum of the operator Ξ|Φ(H);

    (3) Ξ2 is unitarily equivalent to S00, where S is the g-frame operator of {ΛiU}iI,UU and 00 is the zero operator on Φ(H).

    Proof. Assume that S is the g-frame operator for {ΛiU}iI,UU; then,

    Sf=iI,UUUΛiΛiUf, fH.

    First, we want to prove that SU=US for each UU. In fact, for fH,

    USf=UiI,VUVΛiΛiVf=iI,VUUVΛiΛiVf=iI,VU(UV)ΛiΛi(UV)Uf=SUf.

    Since S is an invertible positive operator, we have that S12U=US12 for each UU. Note that {ΛiB(H,K)}iI is a g-frame generator set for U; we know that {ΛiUS12}iI,UU is a Parseval g-frame (see [7], Remark1). Then, {ΛiS12U}iI,UU is also a Parseval g-frame, that is, {ΛiS12}iI is a Parseval g-frame generator set for U. Let Φ be the analysis operator of the Parseval g-frame {ΛiS12U}iI,UU. Then,

    Φ:H2(I×U)K,
    Φf=iI,UULiUΛiS12Uf, fH.

    Thus, for each fH and UU, we have

    (λUIK)Φf=(λUIK)iI,VULiVΛiS12Vf=iI,VU(λUIK)(eiVΛiS12Vf)=iI,VU(ei(UV)ΛiS12Vf)=iI,VULi(UV)ΛiS12Vf=iI,VULi(UV)ΛiS12(UV)Uf=ΦUf.

    Since {ΛiS12U}iI,UU is a Parseval g-frame, it implies that ΦΦ is the identity on H. This leads to

    Φ(λUIK)Φ=U,

    that is, (1) holds.

    Let Φ be the synthesis operator of {ΛiS12U}iI,UU defined by

    Φ:2(I×U)KH,
    Φ=iI,UUU(ΛiS12)LiU.

    Set Ξ=ΦS12Φ. Then for all UU and gK, one has

    Ξ(eiUg)=ΦS12Φ(eiUg)=ΦS12iI,VUV(ΛiS12)LiV(eiUg)=ΦS12iI,VUV(ΛiS12)eiU,eiVg=ΦS12US12Λig=ΦUΛig.

    Since any element in Φ(H) can be expressed as iI,UU(eiUΛiS12Uf) for fH, we have

    ΞiI,UU(eiUΛiS12Uf)2=iI,UUΞ(eiUΛiS12Uf)2=iI,UUΦUΛiΛiS12Uf2=iI,UUUΛiΛiS12Uf2=iI,UUUΛiΛiUS12f2=S12f2=Sf,f.

    This implies that

    Af2ΞiI,UU(eiUΛiS12Uf)2Bf2.

    Since, for any fH, Φf=iI,UU(eiUΛiS12Uf) and Φ is an isometric operator, it follows that

    f2=iI,UU(eiUΛiS12Uf)2.

    Let g=iI,UU(eiUΛiS12Uf). It turns out that

    Ag2Ξg2Bg2    gΦ(H),

    which proves (2).

    Finally, to verify (3), we define U0:HΦ(H)2(I×U)K by

    U0h={Φh,hH,h,  hΦ(H).

    Obviously, U0 is unitary because Φ is an isometric operator. Since ΦΦ is the identity on H and Ξ=ΦS12Φ, we get that

    Ξ2=ΦS12ΦΦS12Φ=ΦSΦ.

    Then,

    Ξ2U0h={Ξ2Φh=ΦSh=U0Sh,       hH,Ξ2h=ΦSΦh=0=U000h,hΦ(H),

    Thus, Ξ2=U0(S00)U0. The proof is complete.

    Corollary 2.5. Suppose that U is a unitary group on Hilbert space H and {ΛiB(H,K)}iI is a g-frame generator set for U with the frame bounds A and B. Then,

    (1) there exists a Hilbert space NH and a unitary group V on N such that the restriction map VVV|H is a group isomorphism of V onto U;

    (2) there exists a positive operator Ξ:NH such that

    {A12,B12}σ(Ξ|H)[A12,B12].

    Proof. Let N=2(I×U)K. By Theorem 2.4(1), we know that Φ(H) is an invariant subspace of λUIK and Φ is an isometric operator, where Φ is defined as in Theorem 2.4. So, we can embed H into N by identifying H with Φ(H). Denote V={λUIK}UU. Then, clearly, V is a unitary group on N. Hence, the restriction map VVV|H is a group isomorphism of V onto U. By Theorem 2.4(2), it is easily seen that (2) holds.

    In this section, we survey the dilation property of g-frames in the context of projective unitary representations. For this purpose, we need to recall a few concepts and notations, which can be found in [20].

    A projective unitary representation π for a countable group G is a mapping gπ(g) from G into the group U(H) of all unitary operators on a separable Hilbert space H such that

    π(g)π(h)=μ(g,h)π(gh)for all g,hG,

    where μ(g,h) is a scalar-valued function on G×G taking values in the circle group T. The function μ(g,h) is then called a multiplier of π. We also say that π is a μ-projective unitary representation. It is clear from the definition that

    μ(g1,g2g3)μ(g2,g3)=μ(g1g2,g3)μ(g1,g2),g1,g2,g3G, (3.1)
    μ(g,e)=μ(e,g)=1,gG,e is the group unit of G. (3.2)

    Any function μ:G×G(T) satisfying (3.1) and (3.2) above will be called a multiplier for G.

    Similar to the group unitary representation case, the left regular projective representation with a multiplier μ for G plays a crucial role here. Let μ be a multiplier for G. For each gG, we define λg:2(I×G)2(I×G) by

    λgeih=μ(g,h)ei(gh),  hG, (3.3)

    where I is a finite set and {eih}iI,hG is the standard orthonormal basis for 2(I×G). Clearly, λg is a unitary operator on 2(I×G).

    Theorem 3.1. Let G be a countable group and π be a projective unitary representation of G on H with a multiplier μ. Assume that {ΛiB(H,K)}iI is a g-frame generator set for {π(g)}gG. Then,

    (1) there exists a family of operators {CiB(H,K)}iI such that {Ci}iI is a Parseval g-frame generator set for {π(g)}gG;

    (2) there exists an isometry Φ:H2(I×G)K such that Φ(λgIK)Φ=π(g) for all gG;

    (3) there exists a projective unitary representation Δ(g) of G on 2(I×G)K and a family of operators {Λi}iI such that {ΛiΔ(g)}iI,gG is a g-orthonormal basis for 2(I×G)K;

    (4) there exist μ-projective unitary representations π1 and π2 of G on a Hilbert space Φ(H) and Φ(H), respectively, and diagonal Parseval g-frame generator sets {Mih}iI,hG and {Nih}iI,hG for π1(g) and π2(g), respectively, such that {δgh[Mihπ1(g)Nihπ2(g)]}iI,g,hG is a g-orthonormal basis for Φ(H)Φ(H).

    Proof. (1) First, we need to check that π(g)S=Sπ(g) holds for all gG, where S is the g-frame operator for {Λiπ(g)}iI,gG. Indeed, for gG and xH, we have

    π(g)Sx=π(g)(iI,hGπ(h)ΛiΛiπ(h)x)=(iI,hGπ(g)π(h)ΛiΛiπ(h)x)=iI,hGμ(g,h)π(gh)ΛiΛiπ(h)x=iI,hGμ(g,h)π(gh)ΛiΛiπ(h)π(g)π(g)x=iI,hGμ(g,h)π(gh)ΛiΛi(π(g)π(h))π(g)x=iI,hGμ(g,h)¯μ(g,h)π(gh)ΛiΛiπ(gh)π(g)x=Sπ(g)x.

    Thus, π(g)S=Sπ(g), as claimed. Since S is an invertible positive operator, we know that S12π(g)=π(g)S12 for each gG. Since {ΛiB(H,K)}iI is a g-frame generator set for {π(g)}gG, it follows that {ΛiS12π(g)}iI,gG is a Parseval g-frame for H. Let Ci=ΛiS12. Then, it can be verified that Ci satisfies the requirements.

    (2) Let Φ:H2(I×G) be the analysis operator of the Parseval g-frame {Ciπ(g)}iI,gG. Then, for each xH,

    Φx=iI,gG(eigCiπ(g)x),

    where {eig}iI,gG is the standard orthogonal basis of 2(I×G). Obviously, Φ is an isometric operator. Let λg be a unitary operator as defined in (3.3). Since π(g)=¯μ(g,g1)π(g1) and

    (λgIK)(ei(g1h)k)=μ(g,g1h)(eihk), (3.4)

    for each kK, it follows that

    Φπ(g)x=iI,hG(eihCiπ(h)π(g)x)=iI,hG{eihCi[π(g)π(h)]x}=iI,hG{eihCi[¯μ(g,g1)π(g1)π(h)]x}=iI,hG{eihCi[¯μ(g,g1)μ(g1,h)π(g1h)]x}=iI,hG¯μ(g,g1h)μ(g1,h)μ(g,g1){(λgIK)(eg1hCiπ(g1h)x)}=(λgIK)iI,hG(eg1hCiπ(g1h)x)=(λgIK)Φx,

    for each xH. In the penultimate step we used (3.1) and (3.2) to eliminate three multiplier terms. Hence,

    Φ(λgIK)Φ=π(g),  for all gG,

    Thus, (2) is proved.

    (3) Define Δ(g)=λgπ(g). For all h,gG, we have

    Δ(g)Δ(h)=[λgπ(g)][λhπ(h)]=λgλhπ(g)π(h)=[μ(g,h)]2Δ(gh).

    Denote ν(g,h)=[μ(g,h)]2. Then, for any g1,g2,g3G,

    ν(g1g2,g3)ν(g1,g2)=[μ(g1g2,g3)μ(g1,g2)]2=[μ(g1,g2g3)μ(g2,g3)]2=ν(g1,g2g3)ν(g2,g3),
    ν(g,e)=ν(e,g)=1, gG, e is the unit of G,

    and, consequently, Δ is a ν-projective unitary representation of G.

    Let N=2(I×G)K and Λi=(λeΛiS12). Then, for all g,hG, i,jI and k,ki,kjK, we have

        ΛiΔ(g)(eigki),ΛjΔ(h)(ejgkj)=(λeΛiS12)(λgπ(g))(eigki),(λeΛjS12)(λhπ(h))(ejhkj)=δi,jδg,heigki,ejhkj,

    and

         iI,gGΛiΔ(g)(eigk)2=iI,gG(λeΛiS12)(λgπ(g))(eigk)2=iI,gGλgeigΛiS12π(g)k2=iI,gGΛiS12π(g)k2=eigk2.

    Therefore, {ΛiΔ(g)}iI,gG is a g-orthonormal basis.

    (4) Let P be the orthogonal projection onto Φ(H). Then for all xH, kK, gG and jI,

    Φx,P(ejgk)=PΦx,(ejgk)=iI,hG(eihCiπ(h)x),ejgk=Cjπ(g)x,k=x,π(g)Cjk=Φx,Φπ(g)Cjk.

    Hence, {P(ejgk)Φπ(g)Cjk}Φ(H). Since {P(ejgk)Φπ(g)Cjk}Φ(H), it implies that

    P(ejgk)=Φπ(g)Cjk. (3.5)

    Using (3.4) and (3.5), for jI, hG and kK, we deduce that

    (λgIK)P(ejhk)=(λgIK)Φπ(h)Cjk=(λgIK)iI,vG(eivCiπ(v)π(h)Cjk)=iI,vGμ(g,v)(ei(gv)Ciπ(v)π(h)Cjk))=iI,vGμ(g,v)(ei(gv)Ci(π(g)π(v))π(g)π(h)Cjk))=iI,vG(ei(gv)Ciπ(gv)π(g)π(h)Cjk))=μ(g,h)Φπ(gh)Cjk=μ(g,h)P(ej(gh)k)=P(λgIK)(ejhk).

    Thus, we get the commutation relation

    (λgIK)P=P(λgIK),for all gG.

    Let Mig=λeΛiS12π(g)(IP) and π1(h)=(IP)(λhIK), where e is the unit of G, iI and g,hG. Then,

    δghMigπ1(h)=δgh(λeΛiS12π(g))(IP)(λhIK)(IP)=δgh(λhΛiS12π(g))(IP)={(IP)(λgπ(g)S12Λi)}.

    Since (IP) is an orthogonal projection, we know that {δghMigπ1(h)}iI,g,hG is a Parseval g-frame for Φ(H). For g,hG, we have

    π1(g)π1(h)=(IP)(λgIK)(λhIK)=(λghIK)(IP)=μ(g,h)(λghIK)=μ(g,h)π1(gh).

    By restricting the domain of π1(g) to Φ(H), we can get that π1 is a μ-projective unitary representation of G on Φ(H). For each iI and g,hG, let Nig=λeΛiS12π(g) and π2(h)=Φπ(h)Φ. Obviously, π2 is a μ-projective unitary representation of G on Φ(H). Moreover, we have

    δghNigπ2(h)=δgh[λeΛiS12π(g)]Φπ(h)Φ=δgh[λeΛiS12π(g)]ΦΦ(λhIK)ΦΦ=δgh[λhΛiS12π(g)]P=[P(λgπ(g)S12Λi)].

    Hence, {δghNigπ2(h)}iI,g,hG is a Parseval g-frame for Φ(H). Thus,

    λeΛiS12π(h)=δgh[(λeΛiS12π(h))P+(λeΛiS12π(h))(IP)]=δgh[Nihπ2(g)Mihπ1(g)].

    By (3), it is easy to see that {δgh[Mihπ1(g)Nihπ2(g)]}iI,g,hG is a g-orthonormal basis. This completes the proof.

    This section is devoted to investigating the g-frame with the structure of projective unitary representations. We will see that the g-frame generators for a projective unitary representation can be characterized from the perspective of complete wandering operators and operators in the commutant of {π(g)}gG.

    Definition 4.1. ([21]) Let U be a unitary system. A complete wandering operator for U is a co-isometry AB(H,K) such that AU={AU:UU} is a g-orthonormal basis for H.

    Let QB(H) be a set. The notation Q will denote the usual commutant of Q, that is,

    Q={TB(H):TQ=QT for QQ}.

    It is well known that, if TB(H) has closed range, then there exists an operator TB(H) such that

    N(T)=R(T),  R(T)=N(T)and  TTy=y,  yR(T),

    where R(T) and N(T) denote the range and null space, respectively. This operator is uniquely determined by these properties, and we call it the pseudo-inverse of T. Clearly, if T is invertible, then T1=T.

    Theorem 4.2. Suppose that G is a countable group, π is a projective unitary representation of G on H with a multiplier μ, and TB(H,K) is a complete wandering operator for {π(g)}gG. Then,

    (1) an operator AB(H,K) is a g-frame generator for {π(g)}gG if and only if there exist an isometric operator Θ{π(g)}gG and an invertible positive operator E{π(g)}gG such that A=TΘE. In particular, an operator A is a Parseval g-frame generator for {π(g)}gG if and only if there exists an isometric operator Θ{π(g)}gG such that A=TΘ;

    (2) if A is a g-frame generator for {π(g)}gG, then there exists a Hilbert space M and an invertible positive operator E{π(g)}gG such that {AE1π(g)}gG is a g-orthonormal basis for M;

    (3) an operator A is a complete wandering operator for {π(g)}gG if and only if there exists a unitary operator U such that U{π(g)}gG and A=TU.

    Proof. (1) Assume that A is a g-frame generator for {π(g)}gG; then, there exist two constants C,D with 0<CD< such that

    Cf2gGAπ(g)f2Df2, fH.

    Let S be the g-frame operator of {Aπ(g)}gG. Then {Aπ(g)S12}gG is a Parseval g-frame. Similar to the proof of Theorem 3.1(1), we can get that Sπ(g)=π(g)S for all gG. Hence, S12{π(g)}gG. It shows that AS12 is also a Parseval g-frame generator for {π(g)}gG. Since T is a complete wandering operator for {π(g)}gG, it follows that

    gGπ(g)T(AS12π(g)f)2=gGAS12π(g)f2=f2, fH.

    Define a bounded linear operator ϕ:HH by

    ϕf=gGπ(g)TAS12π(g)f, fH. (4.1)

    It is easy to see that ϕ is isometric on H. Next we show that ϕ{π(g)}gG. For all hG and fH, we have

    π(h)ϕf=π(h)gGπ(g)TAS12π(g)f=gGμ(h,g)π(hg)TAS12π(g)π(h)π(h)f=gGμ(h,g)π(hg)TAS12[π(h)π(g)]π(h)f=gGπ(hg)TAS12π(hg)π(h)f=ϕπ(h)f.

    Similarly, we can obtain that ϕ{π(g)}gG. Let P be the orthogonal projection onto ϕ(H). Then, for each f1, f2H,

    ϕf1,Pf2=ϕf1,f2=f1,ϕf2=ϕf1,ϕϕf2.

    Hence, ϕϕf2=Pf2. Note that ϕ{π(g)}gG and ϕ{π(g)}gG. Thus,

    Pπ(g)=π(g)P, gG.

    For each fH, kK and gG, we have

    ϕf,Pπ(g)Tk=ϕf,π(g)Tk=hGπ(h)TAS12π(h)f,π(g)Tk=AS12π(g)f,k=f,π(g)S12Ak=ϕf,ϕπ(g)S12Ak.

    Therefore, ϕπ(g)S12Ak=Pπ(g)Tk. Since ϕ{π(g)}gG, P{π(g)}gG and P=ϕϕ, it implies that AS12=Tϕ. That is,

    A=TϕS12.

    Just let Θ=ϕ and E=S12. Then, the conclusion holds.

    Conversely, we first prove that π(g)Θ=Θπ(g), gG. Since π is a projective unitary representation of G on H with a multiplier μ, we have

    π(g)π(g1)=μ(g,g1)π(e)π(g)=¯μ(g,g1)π(g1), gG.

    Observing that Θ{π(g)}gG and π(g1){π(h)}hG, we obtain

    π(g)Θ=Θπ(g)  and  π(g)E=Eπ(g).

    Thus, for all fH and gG,

    gGAπ(g)f2=gGTΘEπ(g)f2=gGTπ(g)ΘEf2=ΘEf2=Ef21E12E1Ef2=1E12f2.

    Combining this with the fact that

    gGAπ(g)f2=gGTΘEπ(g)f2=gGTπ(g)ΘEf2=ΘEf2=Ef2E2f2,

    for each fH and gG, we have

    1E12f2gGAπ(g)f2E2f2, fH,

    that is A is a g-frame generator for {π(g)}gG.

    Specially, if A is a Parseval g-frame generator for {π(g)}gG, then its g-frame operator S is an identity operator on H. Analogous to the above proof, it is easy to see that the result is verified.

    (2) Since T is a complete wandering operator for {π(g)}gG, it follows T is an isometry; thus, there exists a bounded operator T such that TT=I. By (1), we know that {AS12π(g)} is a Parseval g-frame, AS12=Tϕ, and P=ϕϕ. Hence, for all g,hG and f,gK,

    π(g)(AS12)f,π(h)(AS12)g=π(g)ϕTf,π(h)ϕTg=π(g)PTf,π(h)PTg.

    Let M={Tx:xK,TxP(H)}. Obviously, M is a Hilbert space and MH. Then, for f1,f2T(M),

    π(g)PTf1,π(h)PTf2=π(g)Tf1,π(h)Tf2=δghf1,f2.

    Taking E=S12, we have that π(g)(AE1)f1,π(h)(AE1)f2=δghf1,f2 and {AE1π(g)}gG is a Parseval g-frame on M. This shows that {AE1π(g)} is a g-orthonormal basis for M.

    (3) Let ϕ be the operator defined in (4.1). If A is a complete wandering operator for {π(g)}gG, we know that the g-frame operator S is an identity operator on H. Then,

    ϕf=gGπ(g)TAπ(g)f, fH.

    Write U=ϕ. By the proof of (1), we have that UU=I, U{π(g)}gG, and A=TU. Hence, U is a unitary operator for H since A is a complete wandering operator. The other direction is trivial.

    From the above theorem, we immediately have the following consequence.

    Corollary 4.3. Let U be a unitary group on the finite dimensional Hilbert spaces denote by H and TB(H,K) be a complete wandering operator for U. If AB(H,K) is a g-frame generator for U, then there exists an invertible operator E such that EU and AE1 is a complete wandering operator for U.

    In what follows, we will construct complete wandering operators through the use of g-frame generators.

    Theorem 4.4. Let G be a countable group, π be a projective unitary representation of G on H with a multiplier μ, and TB(H,K) be the complete wandering operator for {π(g)}gG. If AB(H,K) is a g-frame generator for {π(g)}gG, then BB(H,K) exists as a g-Bessel sequence generator for {π(g)}gG and a Hilbert space N such that AS12B is a complete wandering operator for {π(g)π(g)}gG on N, where S is the g-frame operator of {Aπ(g)}gG.

    Proof. Assume that T is a complete wandering operator for {π(g)}gG and A is a g-frame generator for {π(g)}gG. Define θ:HH by

    θf=gGπ(g)TAS12π(g)f, fH.

    Then, θ is an isometry. Similar to the proof of Theorem 4.2(1), we obtain that for each hG,π(h)θ=θπ(h). Let P be the orthogonal projection from H onto θ(H). For all f1,f2H we have

    θf1,Pf2=θf1,f2=gGπ(g)TAS12π(g)f1,f2=f1,gGπ(g)(AS12)Tπ(g)f2=θf1,θ[gGπ(g)(AS12)Tπ(g)f2].

    Hence, Pf2=θ[gGπ(g)(AS12)Tπ(g)f2]. Therefore, for each fH and hG,

    π(h)Pf=π(h)θgGπ(g)(AS12)Tπ(g)f=θgGπ(h)π(g)(AS12)Tπ(g)f=θgGπ(hg)(AS12)Tπ(hg)π(h)f=Pπ(h)f.

    Also, we have that (IP)π(h)=π(h)(IP), hG. Set B=T(IP)B(H,K). Then,

    gGBπ(g)f2=gGT(IP)π(g)f2=gGTπ(g)(IP)f2=(IP)f2f2,  fH.

    It implies that B is a g-Bessel sequence generator for {π(g)}gG.

    Denote N=H(θ(H)). Next, we show that AS12B is a Parseval g-frame generator for {π(g)π(g)}gG. For any gG,f1H and f2(θ(H)), we can get

    gG(AS12B)(π(g)π(g))(f1f2)2=gGAS12π(g)f1+Bπ(g)f22=gGAS12π(g)f12+gGBπ(g)f22+2RegGAS12π(g)f1,Bπ(g)f2.

    Applying Theorem 4.2, we have that AS12=Tθ and P=θθ. So,

    gGAS12π(g)f1,Bπ(g)f2=gGTθπ(g)f1,Bπ(g)f2=gGTπ(g)θf1,Tπ(g)(IP)f2=gG(Tπ(g)θf1,Tπ(g)f2Tπ(g)θf1,Tπ(g)Pf2)=θf1,f2θf1,θθf2=0.

    Then,

    gG(AS12B)(π(g)π(g))(f1f2)2=gGAS12π(g)f12+gGBπ(g)f22=f12+f22=f1f22.

    This proves that {AS12π(g)Bπ(g)}gG is a Parseval g-frame.

    On the other hand, for all gG, we have

    π(g)(AS12)π(g)B=θπ(g)Tπ(g)(IP)T=θPπ(g)Tπ(g)(IP)T=[θ(IP)][Pπ(g)T(IP)π(g)T].

    Moreover, for any g,hG and k1,k2K, we obtain

    [π(g)(AS12)π(g)B]k1,[π(h)(AS12)π(h)B]k2=[θ(IP)][Pπ(g)T(IP)π(g)T]k1,[θ(IP)][Pπ(h)T(IP)π(h)T]k2=[Pπ(g)T(IP)π(g)T]k1,[Pπ(h)T(IP)π(h)T]k2=π(g)Tk1,π(h)Tk2=δg,hk1,k2.

    In the last step, we applied T as a complete wandering operator for {π(g)}gG. Hence, AS12B is a complete wandering operator for {π(g)π(g)}gG on N.

    Remark 4.5. If H is a finite dimensional Hilbert space, by the proof of Theorem 4.4, we see that θ is a unitary operator. Then, θθ=θθ=I and P=I. Hence, B=T(PI)=00, which is a trivial result.

    For example, let g1=[1001],g2=[1001], and G={g1,g2}B(C2). Let H=C2,K=span{eg1}, and the projective unitary representation π(gi)egj=egigj, where i,j=1,2 and egi takes the value of 1 at i and zero elsewhere. Clearly, for any fH, Tf=f,eg1eg1 is a complete wandering operator for π(G), Af=f,eg2eg1 is a Parseval g-frame generator of π(G), and S=I. Then, for any fH, we have that θf=f,eg1eg2+f,eg2eg1. It follows that P=θθ=I and B=T(IP)=00. Hence, A00 is a complete wandering operator for {π(g)π(g)}gG.

    As we know, one of the essential applications of frames is that they lead to expansions of vectors in the underlying Hilbert space in terms of the frame elements. Dual frames play a key role in this decomposition. So, in this section, we mainly consider the dual g-frame generators for projective unitary representations and give some of their characterizations. We first review the definition of dual g-frames.

    From [9, Definition 3.1], a g-Bessel sequence {ΓjB(H,K)}jJ is called a dual g-frame for a g-Bessel sequence {ΛjB(H,K)}jJ if

    f=jJΛjΓjf, fH.

    If S is the g-frame operator for {ΛjB(H,K)}jJ, then {ΛjS1}jJ is a dual for {Λj}jJ and is called the canonical dual g-frame of {Λj}jJ.

    For our purpose, and motivated by the above definition, we introduce the following concept.

    Definition 5.1. Let G be a countable group and π be a projective unitary representation of G on H with a multiplier μ. Two g-Bessel sequence generators A,BB(H,K) for {π(g)}gG are called dual g-frame generators if

    f=gGπ(g)ABπ(g)f, fH.

    Let θ1 and θ2 be the analysis operators for the g-Bessel sequences {Aπ(g)}gG and {Bπ(g)}gG, respectively. Then, for all fH, we have

    f4=|f,f|2=|gGπ(g)ABπ(g)f,f|2=|θ1f,θ2f|2θ1f2θ2f2θ22f2θ1f2=θ22f2gGAπ(g)f2,

    that is Aπ(g)21θ22f2. This shows that A is a g-frame generator for {π(g)}gG. Similarly, B is a g-frame generator for {π(g)}gG. Hence, we also say that A and B form a g-frame generator dual pair for {π(g)}gG. Moreover, if S is the g-frame operator for the g-frame {Aπ(g)}gG, then {AS1π(g)}gG is a dual g-frame for {Aπ(g)}gG. We call AS1 the canonical dual g-frame generator of {Aπ(g)}gG.

    Analogous to [9, Lemma 3.2], we give some elementary characterizations of duals in terms of the analysis operators.

    Proposition 5.2. Let A and B be two g-frame generators for {π(g)}gG with analysis operators θ1 and θ2, respectively. Then, the following statements are equivalent:

    (1) A and B are g-frame generator dual pairs.

    (2) θ2θ1=I.

    (3) θ1θ2=I.

    Proof. (1)(2) Since, for any fH,

    θ1f=gGegAπ(g)f  and  θ2f=hGehBπ(h)f,

    where {eg}gG is the orthonormal basis for 2(G), it follows that

    θ2θ1f=gGπ(g)BAπ(g)f=f.

    Hence, θ2θ1=I.

    (2)(3) and (3)(1) are obvious.

    Theorem 5.3. Let G be a countable group, π be a projective unitary representation of G on H with a multiplier μ and TB(H,K) be a complete wandering operator for {π(g)}gG. Then, A,BB(H,K) are g-frame generator dual pairs for {π(g)}gG if and only if there exist isometric operators Θ1, Θ2{π(g)}gG and invertible positive operators E1, E2{π(g)}gG such that A=TΘ1E1, B=TΘ2E2, and (Θ1E1)(Θ2E2)=I.

    Proof. Suppose that A and B are g-frame generator dual pairs for {π(g)}gG. By Theorem 4.2, we know that there exist isometric operators Θ1, Θ2{π(g)}gG and invertible positive operators E1,E2{π(g)}gG such that A=TΘ1E1 and B=TΘ2E2. The hypothesis that A and B are g-frame generator dual pairs implies that

    gGπ(g)ABπ(g)f=gGπ(g)(TΘ1E1)TΘ2E2π(g)f=f, fH. (5.1)

    Since Θ1,Θ2{π(g)}gG,E1,E2{π(g)}gG, it follows that Θiπ(g)π(g)=π(g)Θiπ(g),i=1,2. So,

    Θiπ(g)=π(g)Θi  and  Θiπ(g)=π(g)Θi,i=1,2.

    Also, we have

    Eiπ(g)=π(g)Ei  and  Eiπ(g)=π(g)Ei, i=1,2.

    Therefore, (5.1) becomes

    gGπ(g)ABπ(g)f=(Θ1E1)gGπ(g)TTπ(g)(Θ2E2)f=(Θ1E1)(Θ2E2)f=f,

    which means that (Θ1E1)(Θ2E2)=I.

    The other direction is clear.

    In this paper, we extend the dilation theorem to g-frames with some additional structure and give some characterizations of g-frame generators for projective unitary representation in terms of complete wandering operators. Moreover, we introduce the notion of dual g-frame generators and obtain some characterizations of the g-frame generator dual pairs.

    Aifang Liu: Conceiving and refining the ideas of the study, Formal analysis, Writing-review and editing; Jian Wu: Writing-original draft preparation, Formal analysis. All authors have read and agreed to the published version of the manuscript.

    The authors declare that they have not used artificial intelligence tools in the creation of this article.

    This work was partially supported by the National Natural Science Foundation of China (No. 11801397).

    We declare that there are no conflicts of interest.



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