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ON SOME PROPERTIES OF CONTINUOUS G-FRAMES AND RIESZ-TYPE CONTINUOUS G-FRAMES

Mohammad Reza Abdollahpour and Yavar khedmati

Department of Mathematics, Faculty of Sciences,

University of Mohaghegh Ardabili, Ardabil 56199-11367, Iran

e-mails: [email protected]; [email protected];

[email protected], [email protected]

(Received 6 October 2015; accepted 31 March 2016)

In this paper we provide some necessary and sufficient conditions under which, a family of bounded operators is a continuousg-frame (Riesz-type continuous g-frame). Also, we study stability of duals of continuousg-frames.

Key words : Continuous frame; continuousg-frame; Riesz-type continuousg-frame.

1. INTRODUCTION

In 1952, the concept of frames for Hilbert spaces was defined by Duffin and Schaeffer [4]. Frames

are important tools in the signal processing, image processing, data compression, etc. In 1993, Ali et

al., [2] developed the notion of ordinary frame to a family indexed by a measurable space which are

known as continuous frames.

Definition 1.1 — LetHbe a complex Hilbert space and(Ω, µ)be a measure space. A mapping

F : Ω→ His called a continuous frame with respect to(Ω, µ), if

(i) F is weakly-measurable, i.e., for allf ∈ H,ω→ hf, F(ω)iis a measurable function onΩ,

(ii) there exist constantsAF, BF >0such that

AFkfk2

Z

|hf, F(ω)i|2(ω)≤BFkfk2, f ∈ H.

In 2006, g-frames or generalized frames introduced by Sun [6] and Abdollahpour and Faroughi

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of this paper we assume thatHis a complex Hilbert space and(Ω, µ)is a measure space with positive

measureµand{Kω : ω }is a family of Hilbert spaces. Now, we summarize some facts about

continuousg-frames from [1].

We say that F Qω∈ is strongly measurable if F as a mapping of Ω to

L

ω∈ is

measurable, where

Y

ω∈=

(

f : Ω [ ω∈

:f(ω)∈ Kω

)

.

Definition 1.2 — We say thatΛ = {Λω B(H,Kω) : ω }is a continuousg-frame forH

with respect to{Kω:ω }if

(i) for eachf ∈ H,{Λωf :ω∈}is strongly measurable,

(ii) there are two constants0< AΛ≤BΛ<∞such that

AΛkfk2

Z

kΛω(f)k2(ω)≤BΛkfk2, f ∈ H. (1.1)

We call AΛ, BΛ the lower and upper continuous g-frame bounds, respectively. Λ is called a

tight continuousg-frame ifAΛ = BΛ,and a Parseval continuousg-frame ifAΛ = BΛ = 1.If for

eachω ,K = Kω,then Λ is called a continuousg-frame forH with respect to K. A family

Λ = {Λω B(H,Kω) : ω } is called a continuous g-Bessel family for H with respect to {Kω :ω }if the right hand inequality in (1.1) holds for allf ∈ H. In this case,BΛis called the

Bessel constant.

If there is no confusion, we use continuousg-frame (continuousg-Bessel family) instead of

con-tinuousg-frame forHwith respect to{Kω:ω∈}(continuousg-Bessel family forHwith respect

to{Kω :ω∈}).

Proposition 1.3 [1] — LetΛ = {Λω B(H,Kω) : ω } be a continuous g-frame. There

exists a unique positive and invertible operatorSΛ:H → Hsuch that for eachf, g∈ H

hSΛf, gi=

Z

hf,ΛωΛωgidµ(ω), f, g∈ H,

andAΛI ≤SΛ ≤BΛI.

The operatorSΛin Proposition 1.3 is called the continuousg-frame operator ofΛ.Also, we have

hf, gi =

Z

hSΛ1f,ΛωΛωgidµ(ω)

=

Z

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We consider the space

b

K =

(

F Y ω∈

:F is strongly measurable,

Z

kF(ω)k2(ω)<∞

)

.

It is clear thatKbis a Hilbert space with point wise operations and the inner product given by

hF, Gi=

Z

hF(ω), G(ω)idµ(ω).

Proposition 1.4 [1] — LetΛ = {Λω B(H,Kω) : ω }be a continuous g-Bessel family.

Then the mappingTΛ:K → Hb defined by

hTΛF, gi=

Z

hΛωF(ω), gidµ(ω), F ∈Kb, g∈ H, (1.3)

is linear and bounded withkTΛk ≤

BΛ.Also, for eachg∈ Hwe have

TΛ(g)(ω) = Λωg, ω∈.

Theorem 1.5 [1] — Let(Ω, µ)be a measure space, whereµisσ-finite. Suppose thatΛ ={Λω B(H,Kω) : ω }is a family of operators such that{Λωf : ω }is strongly measurable, for

eachf ∈ H.ThenΛis a continuousg-frame if and only if the operatorTΛ:K → Hb defined by (1.3)

is a bounded and onto operator.

The operatorsTΛandTΛin Theorem 1.8 are called synthesis and analysis operators ofΛ,

respec-tively.

Definition 1.6 — LetΛ ={Λω ∈B(H,Kω) :ω∈}andΘ ={Θω ∈B(H,Kω) :ω }be

two continuousg-frames such that

hf, gi=

Z

hf,ΘωΛωgidµ(ω), f, g∈ H,

thenΘis called a dual continuousg-frame ofΛ.

LetΛ ={Λω ∈B(H,Kω) :ω∈}be a continuousg-frame. ThenΛ =e {ΛωSΛ1 ∈B(H,Kω) : ω }is a continuousg-frame and by (1.2),Λe is a dual of Λ.we callΛe the canonical dual ofΛ.

One can always get a tight continuousg-frame from any continuousg-frame, in fact, ifΛ ={Λω B(H,Kω) : ω } is a continuous g-frame for Hthen {ΛωSΛ1/2 B(H,Kω) : ω } is a

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Definition 1.7 — LetΛ ={Λω ∈B(H,Kω) :ω }andΘ ={Θω ∈B(K,Kω) :ω }be

two continuousg-frames. ThenΛandΘare said similar if there is an invertible operatorS:H → K

such thatΘωS = Λωfor a.e.ω .

Two continuousg-Bessel familiesΛ ={Λω∈B(H,Kω) :ω∈}andΘ ={Θω∈B(H,Kω) : ω∈}are weakly equal, if for allf ∈ H,

Λωf = Θωf, a.e. ω∈.

Proposition 1.8 [1] — LetΛ ={Λω ∈B(H,Kω) :ω∈}andΘ ={Θω∈B(K,Kω) :ω∈}

be two continuousg-frames. ThenΛandΘare similar if and only if their analysis operators have the

same ranges (weakly).

If the continuous g-frameΛ = {Λω B(H,Kω) : ω }have only one dual(weakly), i.e.,

every dual ofΛis weakly equal to the canonical dual ofΛ, thenΛis called a Riesz-type continuous

g-frame.

Theorem 1.9 — LetΛ = {Λω B(H,Kω) : ω } be a continuousg-frame. ThenΛ is a

Riesz-type continuousg-frame if and only ifRangeTΛ =Kb.

2. SOMENEWRESULTS FORCONTINUOUSG-FRAMES

In this section by generalizing some results of [5], we give some necessary and sufficient conditions

that a family of bounded operators{Λω ∈B(H,Kω) :ω }is a continuousg-frame (Riesz-type

continuousg-frame). In this section until the end of Proposition 2.5,is a finite dimensional Hilbert

space with orthonormal basis{eω,j :j∈Jω}for allω∈.

Proposition 2.1 — Let{ei}i∈I be an orthonormal basis forHand{eωj}j∈Jω be an orthonormal

basis for, for allω∈Ω. Then the following are equivalent:

(i) Λ ={Λω ∈B(H,Kω) :ω∈}is a Parseval continuousg-frame.

(ii) There exist an orthonormal set{ψi}i∈I Kb such that

P

i∈Ikψi(ω)k2 < for a.e. ω

and for allf ∈ H,

Λωf =

X

i∈I

hf, eiiψi(ω), a.e. ω∈.

PROOF:(i)(ii)We considerψi=TΛ∗ei, for alli∈I. Then

kψik2 = kTΛ∗eik2 =

Z

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and

hψi, ψji = hTΛ∗ei, TΛ∗eji=

Z

hΛωei,Λωejidµ(ω) =hei, eji= 0, i6=j.

On the other hand,

X

i∈I

kψi(ω)k2 =

X

i∈I

kΛωeik2 =

X

i∈I

kX

j∈Jω

hΛωei, eωjieωjk2

= X

j∈Jω

X

i∈I

|hei,Λ∗ωeωji|2=

X

j∈Jω

kΛωeωjk2 <∞.

Furthermore, for anyf ∈ H,

Λωf =

X

i∈I

hf, eiiΛωei =

X

i∈I

hf, eiiψi(ω).

Conversely, since{ψi}i∈I⊆Kbis an orthonormal set then for anyf ∈ H

Z

kΛωfk2(ω) =

Z Ω ° ° °X i∈I

hf, eiiψi(ω)

° ° °2(ω)

= kX i∈I

hf, eiik2

= X

i∈I

|hf, eii|2 =kfk2.

We recall that a Riesz basis for a Hilbert spaceHis a family of the form{U ei}i∈I, where{ei}i∈I

is an orthonormal basis forHandU :H → His a bounded bijective operator. 2

Theorem 2.2 — LetΛω∈B(H,Kω)be given for allω∈.The following are equivalent:

(i) Λ ={Λω ∈B(H,Kω) :ω∈}is a continuous g-frame.

(ii) Λωf =

P

i∈Ihf, eiiψi(ω) for some orthonormal basis {ei}i∈I of H and some family {ψi}i∈I Kb with the property that {ψi}i∈I is a Riesz basis for span{ψi}i∈I and

P

i∈Ikψi(ω)k2 <∞for a.e.ω .

(iii) Λωf =

P

i∈Ihf, hiiψi(ω) for some Riesz basis {hi}i∈I of H and some orthonormal set {ψi}i∈I⊆Kband with the property that

P

i∈Ikψi(ω)k2 <∞for a.e.ω .

(iv) Λωf =

P

i∈Ihf, hiiψi(ω)for some Riesz basis{hi}i∈I ofHand some family{ψi}i∈I Kb

with the property that{ψi}i∈Iis a Riesz basis forspan{ψi}i∈I and

P

i∈Ikψi(ω)k2 <∞for

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PROOF:(i)(ii)Let{ei}i∈Ibe an orthonormal basis ofHandψi =TΛ∗eifor alli∈I. Then

for any finite sequence of scalars{ck},we have

kXckψkk2=k

X

ckTΛ∗ekk2 = kTΛ

¡ X

ckek

¢

k2

=

Z

kΛω

¡ X

ckek

¢

k2(ω),

So

AΛX|ck|2 =AΛkXckekk2 ≤ kXckψkk2

BΛkXckekk2 =BΛX|ck|2.

Therefore, by [3, Theorem 3.6.6],{ψi}i∈Iis a Riesz basis forspan{ψi}i∈I. We also haveΛωf

=Pi∈Ihf, eiiψi(ω)and

P

i∈Ikψi(ω)k2 <∞.

(ii)(i)Since{ψi}i∈I ⊆Kbis a Riesz basis forspan{ψi}i∈I, there existB ≥A >0such that

Akfk2=AX i∈I

|hf, eii|2 ≤ k

X

i∈I

hf, eiiψik2

BX

i∈I

|hf, eii|2 =Bkfk2.

Thus

Akfk2

Z

kΛωfk2(ω) =kX i∈I

hf, eiik2 ≤Bkfk2.

(i)(iii)Let{ei}i∈Ibe an orthonormal basis ofH. By Proposition 2.1, there exists an orthonormal

set{ψi}i∈IinKbsuch that

P

i∈Ikψi(ω)k2 <∞for a.e.ω Ω, and for allg∈ H

ΛωSΛ1/2g=

X

i∈I

hg, eiiψi(ω), a.e. ω∈.

For anyf ∈ Hthere existg∈ Hsuch thatSΛ1/2g=f. Thus

Λωf = ΛωSΛ1/2g=

X

i∈I

hSΛ1/2f, eiiψi(ω) =

X

i∈I

hf, SΛ1/2eiiψi(ω).

It is sufficient to takehi =SΛ1/2ei, for alli∈I.

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hi =U eifor alli∈I. Then for anyf ∈ Hwe have

Z

kΛωfk2(ω) =

Z

kX

i∈I

hf, hiiψi(ω)k2(ω)

= kX i∈I

hf, hiiψik2

= X

i∈I

|hf, hii|2=X

i∈I

|hU∗f, eii|2.

So

kU−1k−2kfk2

Z

kΛωfk2(ω) =X

i∈I

|hf, hii|2 ≤ kUk2kfk2, f ∈ H.

(iv)(i)There existC, D >0such that

Ckfk2 X i∈I

|hf, hii|2≤Dkfk2, f ∈ H.

On the other hand, letB≥A >0be the bounds of Riesz basis{ψi}i∈I.Then

ACkfk2≤AX i∈I

|hf, hii|2 ≤ k

X

i∈I

hf, hiiψik2

=

Z

kX

i∈I

hf, hii(ω)k2(ω)

BX

i∈I

|hf, hii|2 ≤BDkfk2.

for allf ∈ H.According to the(i)(ii)the implication(i)(iv)is obvious. 2

Proposition 2.3 — The following are equivalent:

(i) There exists a Riesz-type continuousg-frameΛ ={Λω ∈B(H,Kω) :ω∈}forH.

(ii) There exist an orthonormal basis{ψi}i∈IforKbsuch that

X

i∈I

kψi(ω)k2 <∞, a.e. ω∈.

(iii) For every orthonormal basis{φi}i∈IforKbwe have

X

i∈I

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PROOF : (i) (ii) By Theorem 2.2,Λωf =

P

i∈Ihf, hiiψi(ω) for some Riesz basis{hi}i∈I

ofH and some orthonormal set{ψi}i∈I Kb with the property that

P

i∈Ikψi(ω)k2 < for a.e. ω∈.By Theorem 1.9, for anyψinKbthere existsf ∈ Hsuch thatTΛ∗f =ψ.Thus

ψ=X

i∈I

hf, hiiψi.

So,span{ψi}i∈I=Kb, therefore{ψi}i∈Iis an orthonormal basis forKb.

(ii)(i)Let us defineΛω ∈B(H,Kω)byΛωf =

P

i∈Ihf, eiiψi(ω)for allω∈,where{ei}i∈I

is an orthonormal basis forH.By Proposition 2.1, Λ = {Λω B(H,Kω) : ω }is a Parseval

continuousg-frame. For anyψinKbwe haveψ=Pi∈Ihψ, ψiiψi.So we have

TΛ³ X j∈I

hψ, ψjiej

´

(ω) = Λω

³ X

j∈I

hψ, ψjiej

´

= X

i∈I

­ X

j∈I

hψ, ψjiej, ei

®

ψi(ω)

= X

i∈I

hψ, ψiiψi(ω) =ψ(ω),

for allω .This means thatTΛis surjective and by Theorem 1.9, the proof is complete. (iii)(ii)It is clear.

(i) (iii) By assumption, Γ = {ΛωSΛ1/2 : ω } is a Parseval continuous g-frame and RangeT∗

Γ = RangeTΛ = Kb. Therefore, TΓ is a surjective isometry and so TΓ is unitary. Let i}i∈Ibe an orthonormal basis forKb. Let us considerei =TΓφi, for alli∈I. Then,{ei}i∈I is an

orthonormal basis forHand

X

i∈I

kφi(ω)k2 =

X

i∈I

k X

j∈Jω

hφi(ω), eωjieωjk2

= X

i∈I

X

j∈Jω

|hφi(ω), eωji|2

= X

i∈I

X

j∈Jω

|hΛωSΛ1/2ei, eωji|2

= X

j∈Jω

X

i∈I

|hei, SΛ1/ωeωji|2

= X

j∈Jω

kSΛ1/ωeωjk2 <∞,

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Corollary 2.4 — LetM be a closed subspace ofKb. Then the following are equivalent:

(i) There exists a continuousg-frameΛ ={Λω∈B(H,Kω) :ω∈}forHandRangeTΛ =M.

(ii) There exist an orthonormal basis{ψi}i∈IforM with the property that

P

i∈Ikψi(ω)k2 <∞,

for a.e.ω∈Ω.

(iii) Every orthonormal basis{φi}i∈I forM satisfies

P

i∈Ikφi(ω)k2 <∞, for a.e. ω∈Ω.

PROOF: (i) (ii) SinceΛ is a continuousg-frame,Γ = {ΛωSΛ1/2 B(H,Kω) : ω }

is a Parseval continuousg-frame. Let{ei}i∈Ibe an orthonormal basis forH.If we takeψi =TΓ∗ei,

for all i I then by Proposition 2.1, {ψi}i∈I is an orthonormal set of M with the property that

P

i∈Ikψi(ω)k2 <∞for a.e.ω∈Ωand

ΛωSΛ1/2g=

X

i∈I

hg, eiiψi(ω), a.e. ω∈, g∈ H.

For anyψ∈M there existsf ∈ Hsuch thatTΛ∗f =ψ.Letg=SΛ1/2f,then

ψ(ω) = Λωf = ΛωSΛ1/2g=

X

i∈I

hg, eiiψi(ω).

(ii)(i)Let{ei}i∈I be an orthonormal basis forH.We define bounded operator

Λω:H → Kω, Λωf =

X

i∈I

hf, eiiψi(ω),

for a.e. ω .Then by Proposition 2.1,Λ ={Λω ∈B(H,Kω) : ω }is a parseval continuous g-frame. Ifψ∈M,thenψ=Pi∈Ihψ, ψiiψiand

TΛ³ X i∈I

hψ, ψiiei

´

(ω) =ψ(ω).

Thus, the proof is complete. (iii)(ii)It is clear.

(i)(iii)Let{φi}i∈Ibe an orthonormal basis forM. LetΓ ={ΛωSΛ1/2 ∈B(H,Kω) :ω },

thenTΓTΓ =TΓ∗TΓ =I.If we takeei=TΓφi,for alli∈Ithen{ei}i∈Iis an orthonormal basis for Hand

X

i∈I

kφi(ω)k2=

X

j∈jω

kSΛ1/ωeωjk

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Proposition 2.5 — Let Λ = {Λω B(H,Kω) : ω } and Θ = {Θω B(H,Kω) : ω } be two continuous g-frames with representation Λωf =

P

i∈Ihf, eiiψi(ω) and Θωf =

P

i∈Ihf, fiiφi(ω)for some{φi}i∈Iand{ψi}i∈IinKb,and for some orthonormal bases{ei}i∈I and {fi}i∈IforH. ThenΛis a dual ofΘif and only if

hψi, φji=hei, fji, i, j∈I.

In particular, ifei=fi, for alli∈I,thenΛis a dual ofΘif and only if{ψi}i∈I and{φi}i∈I are

biorthogonal.

PROOF: For anyf, g∈ Hwe have

hf, gi = X

i,j∈I

hf, eiihfj, gihei, fji,

and

Z

hf,ΛωΘωgidµω =

Z

X

i,j∈I

hf, eiihfj, gihψi(ω), φj(ω)idµ(ω)

= X

i,j∈I

hf, eiihfj, gihψi, φji.

Thus, the proof is completed. 2

In the rest of this section we intend to generalize some results of [7] to continuousg-frame.

Lemma 2.6 — Let (, µ) be a measure space. Let Λ = {Λω B(H,Kω) : ω } and

Θ = {Θω B(H,Kω) : ω } be two Parseval continuous g-frames. Then Range(TΘ) Range(T∗

Λ)if and only if there exists an isometryU :H → Hsuch thatΘω = ΛωU for a.e.ω Ω.

PROOF : Let Range(TΘ) Range(TΛ). RangeTΛ is a closed subspace of Kb. We take

P = T∗

ΛTΛ.So, Range(P) = Range(TΛ).Since Λ is a Parseval continuous g-frame, then P is

an orthogonal projection fromKbontoRange(T∗

Λ).We considerU =TΛTΘ. Then

kU fk2 =hU∗U f, fi=hTΘP TΘ∗f, fi=kfk2, f ∈ H.

and

hU∗f , gi = hTΘTΛ∗f , gi=

Z

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Thus

Z

kωU Θω)fk2(ω) =

Z

kΛωU(f)k2(ω)

Z

hΛωU(f),Θωfidµ(ω)

Z

hΘωf ,ΛωU(f)idµ(ω) +

Z

kΘωfk2(ω)

=kU fk2− hU∗U f , fi − hU f , U fi+kfk2

=kU fk2− kU fk2− kU fk2+kfk2= 0.

Hence,ΛωU f = Θωf for a.e.ω∈Ωandf ∈ H. The other implication is clear. 2

Proposition 2.7 — Let (, µ) be a measure space. LetΛ = {Λω B(H,Kω) : ω }and

Θ = {Θω B(H,Kω) : ω } be two Parseval continuous g-frames and Λ be a Riesz-type

continuousg-frame. ThenΘis Riesz-type if and only if there exists an unitary operatorU :H → K

such thatΘωU = Λω for a.e.ω∈.

PROOF: Let Θ be Riesz-type, thenRange(TΛ) = Range(TΘ) = Kb. By Lemma 2.6, there

is a bounded operatorU on H such that U∗U = IH andΘω = ΛωU for a.e. ω Ωand hence T∗

Θ =TΛ∗U. Since bothTΛandTΘ are invertible, it follows thatU is a unitary operator. For the other

implication, letU :H → Hbe a unitary linear operator such thatΘω = ΛωU, thenTΘ =TΛ∗U and

so,RangeTΘ =Kb. By Theorem 1.9,Θis Riesz-type. 2

Proposition 2.8 — Let Λ = {Λω B(H,Kω) : ω } be a Riesz-type continuousg-frame

andΘ = {Θω ∈B(H,Kω) : ω }be a continuousg-frame. ThenΘis a Riesz-type continuous g-frame if and only ifΛandΘare similar.

PROOF: It is obvious by Proposition 1.8 and Theorem 1.9. 2

Theorem 2.9 — LetΛ = {Λω B(H,Kω) : ω }be a Riesz-type continuous g-frame and

Θ = {Θω B(H,Kω) : ω } be a continuous g-frame. Then the following conditions are

equivalent:

(i) Θis a Riesz-type continuous g-frame.

(ii)There exists a constantM >0such that for allφ∈Kb

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PROOF:(i)(ii)By Proposition 2.8, there is an invertible bounded operatorU :H → Hsuch

thatΘω = ΛωU for a.e.ω .For anyg∈ Handφ∈Kbwe have

hU∗TΛφ, gi = hTΛφ, U gi=

Z

hU∗Λωφ(ω), gidµ(ω)

=

Z

hΘωφ(ω), gidµ(ω) =hTΘφ, gi.

ThenTΘ=U∗TΛand so

kTΛφ−TΘφk2 =kTΛφ−U∗TΛφk2 ≤ kI−U∗k2kTΛφk2

(1 +kUk)2kTΛφk2.

Similarity

kTΛφ−TΘφk2 (1 +kU−1k)2kTΘφk2.

Then we have

kTΛφ−TΘφk2 ≤M.min{kTΛφk2,kTΘφk2}

whereM =max{(1 +kUk)2,(1 +kU−1k)2}.

(ii) (i)Since TΛis invertible, then for any f ∈ H there exists an uniqueφ Kb such that TΛφ=f. Let us consider well defined bounded operatorU :H → Hby

U f =TΘφ, f ∈ H.

By the inequality (2.1), U is injective. On the other hand, since TΘ is surjective, then U is

surjective. So,U is invertible. For anyφ∈Kbandg∈ Hwe have

hφ,{ωΛωU∗)g}ω∈i=

Z

(ω),ωΛωU∗)gidµ(ω)

=

Z

hΘωφ(ω), gidµ(ω)

Z

hΛωφ(ω), U∗gidµ(ω)

=hTΘφ, gi − hTΛφ, U∗gi

=hU TΛφ, gi − hU TΛφ, gi= 0

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3. STABILITY OFDUALS OF CONTINUOUSG-FRAMES

In this section we study stability of duals of continuousg-frames.

Lemma 3.1 — Λ = {Λω B(H,Kω) : ω }be a continuous g-frame and Θ = {Θω B(H,Kω) : ω }is a dual ofΛ. Then there exists a operatorS ∈B(H,Kb)such thatTΛS = 0

andΘωf = (Sf)(ω) + ΛωSΛ1f,for allω Ωandf ∈ H.

PROOF: Let us considerS :H →Kb, by

(Sf)(ω) = Θωf ΛωSΛ1f, f ∈ H, ω∈.

Then for allf ∈ H,

kSfk= (

Z

k(Sf)(ω)k2(ω))1/2

(

Z

kΘωfk2(ω))1/2+ (

Z

kΛωSΛ1fk2(ω))1/2

(pBΘ+1

AΛ)kfk.

Thus,Sis bounded. On the other hand, for anyf, g∈ H,

hTΛSf , gi=

Z

hΛω(Sf)(ω), gidµ(ω)

=

Z

hΛωΘωf , gidµ(ω)

Z

hΛωΛωSΛ1f , gidµ(ω)

=hf, gi − hf, gi= 0.

So,TΛS = 0. 2

Theorem 3.2 — LetΛ ={Λω ∈B(H,Kω) :ω }andΘ ={Θω ∈B(H,Kω) : ω }be

two continuous g-frames. Also, letΛ =ˆ {Λˆω ∈B(H,Kω) :ω }be a fixed dual forΛ. IfΛΘ

is a continuous g-Bessel family with sufficiently small boundε >0, then there exists a dualΘˆ forΘ

such thatΛˆΘˆ is also continuous g-Bessel.

PROOF: By Lemma 3.1, there existS∈B(H,Kb)such thatTΛS= 0and

ˆ

Λωf = (Sf)(ω) + ΛωSΛ1f, f ∈ H, ω .

LetM ={Mω∈B(H,Kω) :ω∈}such that

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It is easy to see thatM is a continuousg-Bessel family with bound(1

AΘ +kSk)

2. Forf, g∈ Hwe

have

hf−TΘTM∗ f , gi=hf, gi −

Z

hΘω(TM f)(ω), gidµ(ω)

=hf, gi −

Z

hΘωMωf , gidµ(ω)

=hf, gi −

Z

hΘω(Sf)(ω), gidµ(ω)

Z

hΘωΘωSΘ1f , gidµ(ω)

=hf, gi − hTΘSf , gi − hf, gi

=−hTΘSf , gi.

Thus,f−TΘTM∗ f =−TΘSf,for allf ∈ H.Hence

kf −TΘTM fk=kTΘSfk=kTΘSf −TΛSfk

≤ kTΘ−TΛkkSkkfk

≤√εkSkkfk,

Therefore, for allf ∈ H,kIH −TΘTM∗ k ≤

εkSkand thus,TΘTM∗ is invertible becauseεis

sufficiently small. Hence,Θ =ˆ {Θˆω B(H,Kω) : ω },Θˆω = (TΘTM )1 is a dual forΘ.

Because

Z

hΘˆωf ,Θωgidµ(ω) =

Z

D

(TM (TΘTM∗ )1f)(ω),Θωg

E

(ω)

=

Z

hTΘTM∗ (TΘTM∗ )1f , gidµ(ω)

=hf, gi.

And we have

kSΛ−SΘk=kTΛTΛ∗−TΛTΘ +TΛTΘ −TΘTΘ∗k

≤ kTΛ−TΘk(kTΛk+kTΘk)

≤√ε(pBΛ+

p

BΘ).

(3.1)

And byΛ(e f) = (Sf)(ω) + ΛωSΛ1f and(f) = (Sf)(ω) + ΘωSΘ1f, we have

hTΛˆφ−TMφ, fi=

Z

(ω),Λˆωfidµ(ω)

Z

(ω), Mωfidµ(ω)

=

Z

(ω),ΛωSΛ1f−ΘωSΘ1fidµ(ω)

=hTΛφ, SΛ1fi − hTΘφ, SΘ1fi

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Hence, by inequality (3.1) we have

kTΛˆφ−TMφk

≤ kTΛφkkSΛ1−S−Θ1k+kTΛ−TΘkkφkkSΘ1k

≤ kTΛkkφkkSΛ1kkSΘ−SΛkkSΘ1k+A1 Θ

εkφk

1

AΛ

1

AΘ

εpBΛ(

p

BΛ+

p

BΘ)kφk+A1 Θ

εkφk

=

ε(AΛ+BΛ+

BΛBΘ) AΛAΘ kφk.

(3.2)

If we takeT = (TΘTM∗ )1, then

kTk ≤ 1

1− kIH −T−1k

1 1−√εS,

and so

kIH −Tk ≤ kTkkIH −T−1k ≤

εkSk

1−√εkSk. (3.3)

Consequently, by inequalities (3.2) and (3.3)

kTΛˆφ−TΘˆφk=supkfk=1|hTΛˆφ−TΘˆφ, fi|

=supkfk=1|h(IH−T∗)TΛˆφ+T∗(TΛˆ −TM)φ, fi|

≤ kIH −T∗kkTΛˆkkφk+kT∗kk(TΛˆ −TM)φk

εkφk 1−√εkSk(kSk

q

BΛˆ +AΛ+BΛ+

BΛBΘ) AΛAΘ ).2

REFERENCES

1. M. R. Abdollahpour and M. H. Faroughi, Continuous G-Frames in Hilbert Spaces, Southeast Asian Bulletin of Mathematics, 32 (2008), 1-19.

2. S. T. Ali, J.-P. Antoine and J.-P. Gazeau, Continuous frames in Hilbert space, Annals of Physics, 222 (1993), 1-37.

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4. R. J. Duffin and A. C. Schaeffer, A class of nonharmonic Fourier series, Transactions of the American Mathematical Society, 72 (1952), 341-366.

5. J.-P. Gabardo and D. Han, Frames associated with measurable space, Advances in Computational Math-ematics, 18 (2003), 127-147.

6. W. Sun,G-frames andg-Riesz bases, Journal of Mathematical Analysis and Applications, 322 (2006), 437-452.

References

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