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Nadia Assila1,M’hamed Ghiati2,Mohammed Mouniane3,Mohamed Rossafi4

1Laboratory of Partial Differential Equations, Spectral Algebra and Geometry, Department of Mathematics, Faculty of Sciences, University of Ibn Tofail, Kenitra, Morocco

2,3Laboratory Analysis, Geometry and Applications Department of Mathematics, Faculty of Sciences, University of Ibn Tofail, Kenitra, Morocco

4LaSMA Laboratory Department of Mathematics Faculty of Sciences, Dhar El Mahraz University Sidi Mohamed Ben Abdellah, P. O. Box 1796 Fez Atlas, Morocco

Email address: 1[email protected],2[email protected],

3[email protected], 4[email protected]

Abstract.

The present paper aims to study c-g-woven for Hilbert C-modules, first, we give some definitions and fundamental properties which will be useful to introduce this notion. And also some of his properties are given. Finally, we discuss the perturbation forc-g-woven.

Keywords: Continuous woveng-frames,g-frames, Hilbert C-modules.

1.Introduction and Preliminaries

Frames generalise orthonormal bases and were introduced by Duffin and Schaefer [7] in 1952 to analyse some deep problems in nonharmonic Fourier series by abstracting the fundamental notion of Gabor [10] for signal processing. In 2000, Frank-larson [8] introduced the concept of frames in HilbetC−modules as a generalization of frames in Hilbert spaces. The basic idea was to consider modules overC−algebras of linear spaces and to allow the inner product to take values in theC−algebras [14]. A. Khosravi and B. Khosravi [12] introduced the fusion frames andg−frame theory in Hilbert C-modules. Afterwards, A. Alijani and M. Dehghan consider frames with C-valued bounds [2] in Hilbert C-modules. N. Bounader and S.

1

Received: 18 January 2023; Accepted: 30 April 2023; Published: 5 May 2023

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Kabbaj [5] and A. Alijani [1] introduced the∗-g-frames which are generalizations of g-frames in Hilbert C-modules. In 2016, Z. Xiang and Y. Li [26] give a generalization of g−frames for operators in Hilbert C-modules. Recently, Fakhr-dine Nhari et al. [15] introduced the concepts of g-fusion frame and K-g-fusion frame in Hilbert C-modules. Bemrose et al. [4]

introduced a new concept of weaving frames in separable Hilbert spaces. This notion has potential applications in distributed signal processing and wireless sensor networks. Weaving Frames in Hilbert C-Modules introduced by X. Zhao and P. Li [29]. For more on frame in HilbertC-modules see [11, 18, 19, 20, 21, 22] and references therein.

We organize the rest of the paper as follows. We continue with this section to collect some definitions, and basic lemmas which will be used in next. In section 2 we introduce the notion of continuousg-woven in Hilbert C-module and discuss some of their properties. In section 3 we discuss perturbation ofc-g-woven.

Throughout this paper, (Ω, µ) is a measure space with positive measureµ,Hand{Hω}ω∈Ω are in HilbertC-module and a family of HilbertC-module, respectively, andU ∈EndA(H,K) is the set of all adjointable operators from H into K. If H = K, then EndA(H,H) will be denoted by H. For each m > 1 where m ∈ N, we define [m] := {1,2, . . . , m} and [m]c={m+ 1, m+ 2, . . .}.

Definition 0.1. [16] LetA be a unitalC-algebra and Hbe a leftA-module, such that the linear structures of A and H are compatible. His a pre-hilbert A-Module if His equipped with an A-valued in product ⟨., .⟩A:H × H → A such that is sesquilinear, positive definite and respects the module action. In the other words,

(i) ⟨x, x⟩A≥0 for allx∈ H and ⟨x, x⟩A = 0 if and only if x= 0.

(ii) ⟨ax+y, z⟩A =a⟨x, z⟩A+⟨y, z⟩A for all a∈ Aand x, y, z ∈ H.

(iii) ⟨x, y⟩A =⟨y, x⟩A for all x, y∈ H.

For x ∈ H we define ∥x∥= ∥⟨x, x⟩A12. If H is complete with ∥.∥, it is called a Hilbert A- module or a Hilbert C-module overA.

For every ain C-algebra A, we have |a|= (aa)12 and the A-valued norm on H is defined by |x|= (xx)12 forx∈ H.

LetHand K be tow Hilbert Amodules, AmapT :H → Kis said to be adjointable if there exists a mapT:K → Hsuch that ⟨T x, y⟩A =⟨x, Ty⟩A for all y∈ K and x∈ H.

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Definition 0.2. [27] Let T ∈ EndA(H,K), then a bounded adjointable operator T ∈ EndA(H,K) is called the Moore–Penrose inverse of T if T TT =T, TT T=T, T T

= T T and TT

=TT.

The notation T is reserved to denote the Moore-Penrose inverse of T. These properties imply thatTis unique andTT andT Tare orthogonal projections. Moreover, Ran T

= Ran TT

,Ran(T) = Ran T T

,Ker(T) = Ker TT

and Ker T

= Ker T T which lead us toK = Ker TT

⊕Ran TT

= Ker(T)⊕Ran T

andH= Ker T

⊕Ran(T).

In [27] Xu and Sheng showed that a bounded adjointable operator between two Hilbert C modules admits a bounded Moore-Penrose inverse if and only if the operator has closed range, we refer the readers to [9, 23, 24] for more detailed information.

Lemma 0.3. [16] Let H and K two Hilbert A-module and T ∈ EndA(H,K). Then, the following assertions are equivalent:

(i) The operator T is bounded andA-linear,

(ii) There exist k >0 such that ⟨T x, T x⟩A ≤k⟨x, x⟩A for allx∈ H.

Lemma 0.4. [3]. Let H and K be two Hilbert A-modules and T ∈EndA(H,K). Then the following statements are equivalent:

(i) T is surjective.

(ii) T is bounded below with respect to norm, i.e., there isτ >0such that∥Tx∥ ≥τ∥x∥, for all x∈ K.

(iii) T is bounded below with respect to the inner product, i.e., there is ζ > 0 such that

⟨Tx, Tx⟩A≥ζ⟨x, x⟩A, for allx∈ K.

Lemma 0.5. [28]Let(Ω, µ)be a measure space,XandY are tow Banach spaces,λ:X →Y be a bounded linear operator and f :Ω→Y measurable function, then

λ(

Z

f dµ) = Z

(λf)dµ.

The following definitions were introduced by M. Rossafi et al. in the paper entitled ”Integral frame in Hilbert C-module” (see [17]). Let (Ω, µ) be a measure space, H and V be two Hilbert C-modules over a unital C-algebra and {Hw}w∈Ω is a family of submodules of EndA(H,Hw) is the collection of all adjointableA-linear maps fromH intoHw.

We define, following:

l2(Ω,{Hw}ω∈Ω) =

F ={Fw}w∈Ω :Fw ∈ Hw, Z

|Fw|2dµ(w)

<∞

.

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For any F = {Fw}w∈Ω and G = {Gw}w∈Ω, the A-valued inner product is defined by

⟨F, G⟩ = R

⟨Fw, GwAdµ(w) and the norm is defined by ∥F∥ = ∥⟨F, F⟩∥12. In this case thel2(Ω,{Hw}ω∈Ω) is an HilbertC-module (see [14]).

Definition 0.6([13]). A family Λ :={Λω∈EndA(H,Hω)}ω∈Ωis called a continuousg-frame (or briefly c−g−frame) in Hilbert A moduleH with respect to{Hω}ω∈Ω if

(i) the mapping

Ω7−→ A

ω7−→ ⟨Λωf,Λωf⟩A is measurable for anyf ∈ H.

(ii) there exist constants 0< A≤B <+∞ such that for eachf ∈ H,

(1) A⟨f, f⟩A

Z

⟨Λωf,Λωf⟩Adµ(ω)≤B⟨f, f⟩A.

IfA,B can be chosen such thatA=B,then{Λω}ω∈Ω is called a tightc−g−frame and if A=B = 1,it is called parseval c-g-frame. A family {Λω}ω∈Ω is calledc−g−Bessel family if the right hand inequality (1) holds and the numberB is called the Bessel constant.

The continuousg−frame operator SΛ on His defined by : SΛ(f) =

Z

ΛwΛwf dµ(w), f ∈ H.

Theorem 0.7. Let{Λω}ω∈Ω be a continuousg−Bessel family inHwith respect to{Hω}ω∈Ω with the bound B. Then the mappingTΛ on l2(Ω,{Hw}ω∈Ω) to His defined by

⟨TΛF, g⟩A = Z

⟨ΛωF(ω), g⟩Adµ(ω), F ∈l2(Ω,{Hw}ω∈Ω), g∈ H, is linear and bounded with∥TΛ∥≤√

B. Furthermore, for each g∈ H and ω∈Ω, TΛ(g)(ω) = Λω(g).

In the continuous g− frame operatorSΛ=TΛTΛ is defined by SΛ:H −→ H,

⟨SΛf, g⟩A= Z

⟨f,ΛωΛωg⟩Adµ.

Therefore,

AI ≤SΛ≤BI

and we obtain, if {Λω}ω∈Ω is a c−g− frame, thenSΛ is positive, self-adjoint and invertible operator.

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Proof. For any F ∈l2(Ω,{Hw}ω∈Ω)

∥TΛF∥= sup

∥g∥=1

∥⟨TΛF, g⟩A∥= sup

∥g∥=1

Z

⟨ΛωF(w), g⟩A

= sup

∥g∥=1

Z

⟨F(w),Λωg⟩A

≤ sup

∥g∥=1

Z

⟨F, F⟩A

1

2

Z

⟨Λωg,Λωg⟩A

1 2

≤√

B∥F∥.

Next, we show thatSΛ is a self-adjoint operator

⟨SΛf, g⟩A =⟨TΛTΛf, g⟩A=⟨f, TΛTΛg⟩A=⟨f, SΛg⟩A Or, by using the notation from opertor theory, we get

AI ≤SΛ≤BI,

thusSΛ is a positive operator furthermore

0≤I−B−1SΛ≤ B−A B I, and consequently

∥I−B−1SΛ∥= sup

∥f∥=1

I−B−1SΛf, f

A

≤ B−A B ≤1,

which shows thatSΛ is inverstible. □

The following Definition is a generalization of the Definition 3.1 in [25], for Hilbert C- modules.

Definition 0.8. A family of c-frames {Fωi}ω∈Ω,i∈[m] in Hilbert C-module H with respect toµ is said to be c-woven if there exist universal same positive constants 0 < A≤B <∞ such that for each partition{σi}i∈[m]of Ω, the family{Fωi}ω∈σi,i∈[m]is ac−frame in Hilbert C-moduleHwith bounds Aand B. Each family {Fωi}ω∈σi,i∈[m] is called a weaving.

2. Continuous weaving g-frames

In this section, we introduce the notation of continuous g-woven in Hilbert C-module and discuss some of their properties.

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Definition 0.9. Two c-g-frames Λ := {Λωi ∈ EndA(H,Hω)}ω∈Ω,i∈[m] and Γ := {Γωi ∈ EndA(H,Hω)}ω∈Ω,i∈[m] are said to be continuous g-woven (or c−g−woven) if there exist universal constants 0< A ≤ B <∞ such that for each partition {σi}i∈[m] of Ω, the family {Λωi}ω∈σi,i∈[m]∪ {Γωi}ω∈σi,i∈[m] is a c−g− frame in Hilbert C-module H with bounds A and B, respectively, that is

(2) A⟨f, fA Z

σ

⟨Λωif,ΛωifAdµ(ω) + Z

σc

⟨Γωif,ΓωifAdµ(ω)B⟨f, f⟩A.

In the above definition,A and B are called universal c-g-frames bounds.

It is easy to show that everyc-g-woven has an universal upper c-g-frame bound.

Indeed, let {Λω}ω∈Ω is be a c-g-Bessel family in Hilbert C-module H with bounds Bi for each i∈[m]. Then, for any partition {σi}i∈[m] of Ω and f ∈ H, we have

X

i∈[m]

Z

σi

⟨Λωif,Λωif⟩Adµ≤ X

i∈[m]

Z

⟨Λωif,Λωif⟩Adµ≤(X

i∈[m]

Bi)⟨f, f⟩A.

In the next results, we construct a c-g-woven by using a bounded linear operator.

Theorem 0.10. Let {Λωi}ω∈Ω,i∈[m] be a c-g- woven in Hilbert C-module H with universal bounds A, B. If T ∈ EndA(H) has closed range, then {ΛωiT}ω∈Ω,i∈[m] is a c−g− woven for R(T) with frame bounds A∥T−2 andB∥T∥2.

Proof. First, since Tf ∈ H and ω 7−→ ⟨Λωif,Λωif⟩A, is measurable for any f ∈ H and i ∈ [m],then ω 7−→ ⟨ΛωiTf,ΛωiTf⟩A, is measurable for any f ∈ H and i ∈ [m]. On the other hand, for eachf ∈ R(T), we have

A∥⟨f, f⟩A∥=A

⟨T Tf, T Tf⟩A

=A∥T Tf∥2

=A∥(T)Tf∥2

≤A∥(T)∥2∥Tf∥2

≤A∥(T)∥2∥⟨Tf, Tf⟩A

≤ ∥(T)∥2

X

i∈[m]

Z

⟨ΛωiTf,ΛωiTf⟩Adµ .

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So,

A∥(T)∥−2∥⟨f, f⟩A∥ ≤

X

i∈[m]

Z

⟨ΛωiTf,ΛωiTf⟩A

≤ X

i∈[m]

Bi∥⟨Tf, Tf⟩A

≤B∥T∥2∥⟨f, f⟩A∥.

□ The following result presents a relationship between the norms of thec-g-frame operator of the originalc-g-frame and the weaving.

Theorem 0.11. Let {Λωi}ω∈Ω,i∈[m] be a c-g-woven in H with universal boundsA and B. If SΛ(i) is the c-g-frame operator of {Λωi}ω∈Ω for each i ∈ [m], SΛ,σi represents the c-g-frame operator of {Λωi}ω∈Ω,i∈[m] for each partition {σi}i∈[m] of and S(i)Λ,σ

i denotes the c-g-frame operatorSΛ(i) with integral restricted to {σi}, then for each f ∈ H,

X

i∈[m]

∥⟨SΛ,σ(i)

if, SΛ,σ(i)

if⟩A∥≤B∥SΛ,σi∥∥⟨f, f⟩A∥.

Proof. Suppose that f ∈ H. We can write X

i∈[m]

∥⟨SΛ,σ(i)

if, SΛ,σ(i)

if⟩A∥= X

i∈[m]

∥SΛ,σ(i)

if∥2

= X

i∈[m]

( sup

∥g∥=1

∥⟨SΛ,σ(i)

if, g⟩A∥)2

= X

i∈[m]

( sup

∥g∥=1

∥⟨TΛ,σ(i)

i(TΛ,σ(i)

i)f, g⟩A∥)2

≤ X

i∈[m]

B∥⟨(TΛ,σ(i)

i)f,(TΛ,σ(i)

i)f⟩A

=B X

i∈[m]

∥ Z

σi

⟨Λωif,Λωif⟩Adµ(ω)∥

≤B∥⟨SΛ,σif, f⟩A

≤B∥SΛ,σi∥∥⟨f, f⟩A∥.

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Theorem 0.12. Let Ωi ⊆ Ω be measurable subsets for all i∈[m], and let Fi and Gi be c-frame mappings on Ωi for Hω with the pair frame bounds (AFi, BFi) and (AGi, BGi) re- spectively, for each ω ∈ Ω. Assume that Λωiωi ∈EndA(H,Ωi), for any i∈[m] such that {Λωi}ω∈Ω,i∈[m] and {Θω∈Ω,i∈[m] are strongly measurable. Then the following assertions are equivalent.

(I) {Λω

iFi}ω∈Ω,i∈[m] and {Θω

iGi}ω∈Ω,i∈[m] arec− woven in Hilbert C-module H.

(II) {Λωi}ω∈Ω,i∈[m] and{Θωi}ω∈Ω,i∈[m] are c−g− woven in Hilbert C-module H.

Proof. (I)⇒(II). Suppose thatσ⊆Ωis measurable subsets andf ∈ H. Let{Λω

iFi}ω∈Ω,i∈[m]

and{Θω

iGi}ω∈Ω,i∈[m]arec-woven inH, with universal frame boundsC, DandA= inf{AFi, AGi}.

Then, for eachi∈[m],we have

A Z

σ

⟨Λωif,Λωif⟩Adµ(ω) +A Z

σc

⟨Θωif,Θωif⟩Adµ(ω)

≤ Z

σ

AFωi⟨Λωif,Λωif⟩Adµ(ω) + Z

σc

AGωi⟨Θωif,Θωif⟩Adµ(ω)

≤ Z

σ

Z

i

|⟨Λωif, Fi(x)⟩A|2dµ(x)dµ(ω) + Z

σc

Z

i

|⟨Θωif, Gi(x)⟩A|2dµ(x)dµ(ω)

= Z

σ

Z

i

|⟨f,ΛωiFi(x)⟩A|2dµ(x)dµ(ω) + Z

σc

Z

i

|⟨f,ΘωiGi(x)⟩A|2dµ(x)dµ(ω)

≤D⟨f, f⟩A.

With the same way, we conclude that

B Z

σ

|⟨Λωif,ΛωifA|2dµ(ω) +B Z

σc

|⟨Θωif,Θωif,A|2dµ(ω)

Z

σ

Z

i

|⟨f,ΛωiFi(x)⟩A|2dµ(x)dµ(ω) + Z

σc

Z

i

|⟨f,ΘωiGi(x)⟩A|2dµ(x)dµ(ω)

C⟨f, fA,

whereB= sup

BFωi, BGωi .Thus, we obtain thatωi}ω∈Ω,i∈[m]andωi}ω∈Ω,i∈[m]arec-g-woven forH with universal frame bounds C

B and D A.

(II) (I). Suppose that ωi}ω∈Ω,i∈[m] and ωi}ω∈Ω,i∈[m] are c-g-woven for H with universal

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frame boundsCand D. Now, we can write for eachf ∈ H,

Z

σ

Z

i

|⟨f,ΛωiFi(x)⟩A|2dµ(x)dµ(ω) + Z

σc

Z

i

|⟨f,ΘωiGi(x)⟩A|2dµ(x)dµ(ω)

= Z

σ

Z

i

|⟨Λωif, Fi(x)⟩A|2dµ(x)dµ(ω) + Z

σc

Z

i

|⟨Θωif, Gi(x)⟩A|2dµ(x)dµ(ω)

Z

σ

AFωi⟨Λωif,ΛωifAdµ(ω) + Z

σc

AGωi⟨Θωif,ΘωifAdµ(ω)

A Z

σ

⟨Λωif,ΛωifAdµ(ω) + Z

σc

⟨Θωif,ΘωifAdµ(ω)

AC⟨f, fA.

Also, we can get

Z

σ

Z

i

⟨f,Λω

iFi(x)⟩Adµ(x)dµ(ω) + Z

σc

Z

i

⟨f,Θω

iGi(x)⟩Adµ(x)dµ(ω)BD⟨f, f⟩A

So,

ΛωiFi ω∈Ω,i∈[m] and

ΘωiGi ω∈Ω,i∈[m] arec-woven forH, with universal boundsAC andBD.

Theorem 0.13. Let {Λωi}ω∈Ω be a c-g-frame in Hilbert C-moduleH with frame bounds Ai

andBi for eachi∈[m]. Suppose that there exists M >0 such that for allf ∈ H, i̸=k∈[m]

and all measurable subset ∆⊂Ω

Z

⟨(Λωi−Λωk)f,(Λωi−Λωk)f⟩Adµ(ω)

≤Mmin

Z

⟨Λωif,Λωif⟩Adµ(ω) ,

Z

⟨Λωkf,Λωkf⟩Adµ(ω)

.

Then, the family{Λωi}ω∈Ω,i∈[m] is a c−g-woven with universal bounds

A

(m−1)(M+ 1) + 1 and B

where, A:=P

i∈[m]Ai andB =P

i∈[m]Bi.

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Proof. The upper bound is evident. For the lower bound, suppose that{σi}i∈[m]is a partition of Ω and f ∈ H.Therefore,

X

i∈[m]

Ai⟨f, f⟩A

X

i∈[m]

Z

⟨Λωif,ΛωifAdµ(ω)

=

X

i∈[m]

X

k∈[m]

Z

σk

⟨Λωif,ΛωifAdµ(ω)

X

i∈[m]

Z

σi

⟨Λωif,ΛωifAdµ(ω)

+ X

k∈[m]

Z

σk

{⟨ΛωifΛωkf,Λωif Λωkfdµ(ω) +⟨Λωkf,ΛωkfAdµ(ω)}

X

i∈[m]

Z

σi

⟨Λωif,ΛωifAdµ(ω) + X

k∈[m]

k̸=i

Z

σk

(M+ 1)⟨Λωkf,ΛωkfAdµ(ω)

={(m1)(M + 1) + 1}

X

i∈[m]

Z

σi

⟨Λωif,ΛωifAdµ(ω) .

3. Perturbation For C-G-Woven

Perturbation of frames has been discussed by Cazassa and Christensen in [6]. For weaving frames, Bemrose and et al. have studied in [4], also Vashisht and Deepshikha presented for continuous case in [25]. We aim to present it forc-g-woven.

Theorem 0.14. Suppose for each i∈[m], the family {Λωi}ω∈Ω is a c−g-frame in H with frame bounds Ai and Bi. Assume that there exist constants λi, ηi and γi(i∈ [m]) such that for some fixedn∈[m],

A:=An− X

i∈[m]\[n]

λii

pBni

pBi

pBn+p Bi

>0 and

Z

Λωn−Λωi

F(w), g

A

ηi

Z

ΛωnF(w), g

A

i

Z

ΛωiF(w), g

A

i∥F∥ for everyF ∈l2(Ω,{Hw}ω∈Ω)andg∈ H.Then for any partition{σj}j∈[m]ofΩ,{Λωi}ω∈σ

j,j∈[m]

is ac-g-frame in HilbertC-Module H with universal frame boundsA and P

i∈[m]Bi. Hence the family of c-g-frame {Λωi}ω∈Ω,i∈[m] is woven in HilbertC-Module H.

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Proof. It is clear that{Λωif}ω∈σ

j,j∈[m]is strongly measurable for eachf ∈ Hand any parti- tion {σj}j∈[m] of Ω, also the family {Λωi}ω∈Ω,i∈[m] is a c-g-Bessel family with Bessel bound P

i∈[m]Bi. Now, we show that {Λωi}ω∈Ω,i∈[m] has the lower frame condition. Assume that TΛi is the synthesis operator of {Λωi}ω∈Ω,i∈[m]. Then for any F ∈ l2(Ω,{Hw}ω∈Ω) for any, i∈[m]\{n}, we have

∥(TΛn −TΛi)F∥= sup

∥g∥=1

⟨(TΛn−TΛi)F(w), g⟩A

= sup

∥g∥=1

⟨TΛnF(w)−TΛiF(w), g⟩A

= sup

∥g∥=1

⟨TΛnF(w), g⟩A− ⟨TΛiF(w), g⟩A

= sup

∥g∥=1

F(w), TΛng

A

F(w), TΛig

A

= sup

∥g∥=1

⟨F(w),Λωng⟩A− ⟨F(w),Λωig⟩A

= sup

∥g∥=1

ΛωnF(w), g

A

ΛωiF(w), g

A

= sup

∥g∥=1

Z

Λωn−Λωi

F(w), g

A

≤ηi sup

∥g∥=1

Z

ΛωnF(w), g

A

i sup

∥z∥=1

Z

ΛωiF(w), g

A

i∥F∥

i∥TΛnF∥+γi∥TΛiF∥+λi∥F∥

≤ηi

pBn∥F∥+γi

pBi∥F∥+λi∥F∥

=

ηi

pBni

pBii

∥F∥.

Thus,

∥TΛn−TΛi∥ ≤ηip

Bnip

Bii. (3)

For eachi∈[m] andσ ⊂Ω, we define

Ti(σ): (⊕ω∈σHω, µ)L2 →H D

Ti(σ)G, hE

A = Z

σ

ΛωiG(w), h

A

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for all G∈l2(Ω,{Hw}ω∈Ω), we have

Ti(σ)G

=∥TΛi(G·χσ)∥

≤ ∥TΛi∥ ∥G·χσ

≤ ∥TΛi∥ ∥F∥2

≤p

Bi∥F∥2

thus, Ti(σ)

≤√

Bi, for eachi∈[m].Similarly with (3), we get for eachi∈[m]\{n},

Tn(σ)−Ti(σ) ≤ηi

pBni

pBii.

For everyf ∈H andi∈[m]\{n}, we compute

Tn(σ) Tn(σ)

−Ti(σ)

Ti(σ) f

Tn(σ) Tn(σ)

−Tn(σ)

Ti(σ) f

+

Ti(σ) Ti(σ)

−Tn(σ)

Ti(σ) f

≤ Tn(σ)

Tn(σ)

Ti(σ) f

+ Ti(σ)

Tn(σ)−Ti(σ) f

≤ ηi

pBni

pBii

pBn+p Bi

∥f∥.

Now, suppose that{σi}i∈[m]is a partition of Ω andTΛbe the synthesis operator associated with thec-g-Bessel family {Λωi}ω∈Ω,i∈[m], we have

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∥TΛf∥2=∥⟨f, TΛTΛf⟩A

=

X

i∈[m]

Z

σi

f,ΛωiΛωif

Adµ(ω)

= Z

σ1

f,Λω1Λω1f

Adµ(ω) +. . .+ Z

σn

f,ΛωnΛωnf

Adµ(ω) +. . . . . .+

Z

σm

f,ΛωmΛωmf

Adµ(ω)

= Z

σ1

f,Λω1Λω1f

Adµ(ω) +. . .+ X

i∈[m]

Z

σi

f,ΛωiΛωif

Adµ(ω)

− X

i∈[m]\{n}

Z

σi

f,ΛωiΛωif

Adµ(ω) + Z

σm

f,ΛωmΛωmf

Adµ(ω)

= Z

f,ΛωnΛωnf

Adµ(ω)−

X

i∈[m]\{n}

Z

σi

f,ΛωnΛωnf

Adµ(ω) − Z

σi

f,ΛωiΛωif

Adµ(ω)

≥ Z

f,ΛωnΛωnf

Adµ(ω)

− X

i∈[m]\(n)

Z

σi

f,ΛωnΛωnf

Adµ(ω)− Z

σi

f,ΛωiΛωif

Adµ(ω)

≥An∥⟨f, f⟩∥A− X

i∈[m]\{n}

D

Tn(σ)

Tn(σ)

f, f E

A−D Ti(σ)

Ti(σ)

f, f E

A

≥An∥⟨f, f⟩∥A− X

i∈[m]\{n}

∥⟨f, f⟩∥A

Tn(σ)

Tn(σ)

−Ti(σ)

Ti(σ)

≥An∥⟨f, f⟩∥A− X

i∈[m]\{n}

∥⟨f, f⟩∥A ηi

pBni

pBii

pBn+p Bi

=A⟨f, f⟩A.

□ Corollary 0.15. For each i ∈ [m], let the family {Λωi}ω∈Ω be a c−g-frame in Hilbert C-module H with frame bounds Ai and Bi. Assume that there exist constants λi, ηi, γi(i∈

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[m−1]) andn∈[m] so that A:=A1− X

i∈[m−1]\{n}

λiip

Biip

Bi+1 p

Bi+p Bi+1

>0 and

Z

D

Λωi−Λω(i+1)

F(w), g E

ηi

Z

ΛωiF(w), g

A

i

Z

D

Λω(i+1)F(w), gE

A

i∥⟨F, F⟩A12, for everyF ∈l2(Ω,{Hw}ω∈Ω)andg∈ H.Then for any partition{σj}j∈[m]ofΩ,{Λωi}ω∈σ

j,j∈[m]

is ac−g-frame in HilbertC-ModuleHwith universal frame boundsAandP

i∈[m]Bi.Hence the family of c-g-frame {Λωi}ω∈Ω,i∈[m] is woven in HilbertC-Module H.

Declarations

Availablity of data and materials Not applicable.

Competing interest

The authors declare that they have no competing interests.

Fundings

The authors declare that there is no funding available fot this paper.

Authors’ contributions

The authors equally conceived of the study, participated in its design and coordination, drafted the manuscript, participated in the sequence alignment, and read and approved the final manuscript.

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