SlideShare a Scribd company logo
1 of 7
Download to read offline
Int. J. Contemp. Math. Sciences, Vol. 6, 2011, no. 36, 1761 - 1767
DENSITY AND INDEPENDENTLY ON Hbc(E)
Parvin Karami
department of mathematics
Islamic Azad University, branch of Mamasani
P.O.Box ..., Mamasani, Iran
karami-pk67@yahoo.com
Mezban Habibi
department of mathematics
Islamic Azad University, branch of Mamasani
P.O.Box ..., Mamasani, Iran
habibi.m@iaudehdasht.ac.ir
Fatemeh Safari
department of mathematics
Islamic Azad University, branch of Mamasani
P.O.Box ..., Mamasani, Iran
safari.s@iaudehdasht.ac.ir
Mohammad Zarrabi
department of mathematics
Islamic Azad University, branch of Mamasani
P.O.Box ..., Mamasani, Iran
m-zarrabi86@yahoo.com
Abstract
The aim of the paper ahead Birhoff , Maclane, Godefroy-Shapiro and
Kitai-Getner-Shapiro and the results of their theorems and hypercyclic
operators on space H(C). In Birhoffs theorem is shown that, if b is
non-zero, then the shift with the vector b is an hypercyclic operator.
Maclane in 1952 showed that the Differentiation operator on H(C) is
an hypercyclic operator. Bourdon and Shapiro also studied the behavior
of operators composition operaotrs on this space. For more information
reader can see [1–14].
2 P. Karami, M. Habibi, F. Safari, M. Zarrabi
Subject Classification: 47A16,47B37
Keywords:Hypercyclic vector, Hypercyclicity criterion, Differentiation op-
erator, Density, Independently, Dual space.
1 Introduction
Let X be a frechet space and T be bounded linear operators on X. For each
x ∈ X put
Orb(T, x) = {Tn
(x) : n ≥ 0)} = {x, Tx, T2
x, T3
x, . . .}
The set Orb(T, x) is called orbit of vector x under the operator T and the
operator T is called hypercyclic operator if there exist vector x in X such that
the set Orb(T, x) is dense in X, that is
Orb(T, x) = {x, Tx, T2x, T3x, . . .} = X.
In this case a vector x is called hypercyclic vector for the operator. If X∗
be the dual of space X and both operators T : X → X and T∗
: X∗
→ X∗
are
hypercyclic, then the operator T is called dual hypercyclic.(Note that if X be
a bounded space, then the dual of X denoted by X ). If M is a subset of X
and all non-zero element of space M be a hpercyclic vector for T, then M is
called hypercyclic subspace of X.
2 Preliminary Notes
Suppose that H(C) be the space of all functions of one complex variable with
the uniform convergence topology on compact subsets of C. Consider Banach
space E, Ferechet algebra by elements of dual space with uniform convergence
topology over the balls of E. Space Hbc(E) containing all bounded functions
on compact subsets of E, the space Hbc(E) includes all functions f = ∞
n=0 Pn
in which
Pn ∈ Span{ϕn : ϕE∗} , n = 0, 1, 2, 3, ...
Pn
1
n = (Sup x <1|Pn|)
1
n → 0 , n → ∞
The operator φ : H(E) → H(E) by definition φ(f) = Df is called differen-
tiation operator. Let ϕ ∈ H(C), then the operator Cϕ : H(C) → H(C) by
definition Cϕ(f) = foϕ on H(C) is hypercyclic, if and only if the operator ϕ
is a shift with a non-zero vector b ∈ C. In other words, ∃0 = b ∈ C, ϕ(z) =
z+b(see[1]). Differentiation operator on H(C) is a hypercyclic operator(see[6]).
running head 3
If φ(z) = |α|≥0 Cαzα
be non-constant entire function on C, Then the oper-
ator φD : H(Cn
) → H(Cn
) by definition φD(f) = |α|≥0 CαDα
f, f ∈ H(C)
is hypercyclic operator(see[10]). Also all continuous linear operator on H(Cn
)
substitute with translation, if and only if, be for one ϕ ∈ H(Cn
) is of expo-
nential form T = ϕ D (see[10]). Let X be an F-space and T : X → X be
a continuous linear operator and assume that X0, Y0 are two dense subsets
of X and {nk}∞
k=1 be a sequence of positive integers, and there are sequences
Snk
: Y0 → X of mapping such that,
(1). Tnk
→ 0, k → ∞ , Pointwise on X0
(2). Snk → 0, k → ∞ , Pointwise on Y0
(3). Tnk
Snk = IY0
then the operator T is hypercyclic(Hypercyclic Creterion)
3 Main Results
Theorem 3.1 The collection B = {eϕ
: ϕ ∈ E∗
} is a independently linear
subset of Hbc(E).
Proof. Let {eϕi
}i∈I be the maximal independently linear subset of B. Sup-
pose ϕ ∈ E∗
be fix point, and ζi1 , ζi2 , ..., ζir ∈ C with the condition,
ζi1 .eϕi1 + ζi2 .eϕi2 + . . . + ζir .eϕir = eϕ
Let α be a trivial element of E. Use the Operator f → df(.)α in bellow
equation, we have,
df(ζi1 .eϕi1 + ζi2 .eϕi2 + . . . + ζir .eϕir )(α) = df(eϕ
)
so
df(ζi1 .eϕi1 )(α) + df(ζi2 .eϕi2 )(α) + . . . + df(ζir .eϕir )(α) = df(eϕ
)(α)
ζi1 .ϕi1 (α).eϕi1 + ζi2 .ϕi2 (α).eϕi2 + . . . + ζir .ϕir (α).eϕir = ϕ(α).eϕ
Since {eϕi
}i∈I is a independently linear subset of B and ζi1 , ζi2 , ..., ζir ∈ C are
non-zero elements, then
ϕi1 (α) = ϕi2 (α) = . . . = ϕir (α)
Now, since α be a trivial element of E, then
ϕi1 = ϕi2 = . . . = ϕir
So {eϕi
}i∈I = C∗
, by this the proof is complete.
4 P. Karami, M. Habibi, F. Safari, M. Zarrabi
Theorem 3.2 Let U be an open subset of E∗
, then S = Span{eϕ
: ϕ ∈ U}
is a dense subset of Hbc(E).
Proof. Let ϕ0 ∈ E∗
and Λ : Hbc(E) → Hbc(E) bye Λ(ψ) = eϕ0
.ψ. Suppose
ψ1, ψ2 ∈ Hbc(E) and Λ(ψ)1 = Λ(ψ)2, so eϕ0
.ψ1 = eϕ0
.ψ2. Since eϕ0
= 0, then
ψ1 = ψ2, that is the operator Λ is one-one operator. Since constant opera-
tor and identity operator are continuous, then the operator Λ is continuous.
Now since Λ(ψ)−1
= e−ϕ0
.ψ is continuous operator, then the operator Λ is a
homeomorphism and
Span{eϕ0+ϕ : ϕ ∈ U} = Hbc(E) ⇔ Span{e+ϕ : ϕ ∈ U} = Hbc(E)
If λo ∈ U then take U0 = {ϕ − λ0 : ϕ ∈ U}, then 0 = λ0 − λ0 ∈ U0, So without
lost of generality we can suppose 0 ∈ U. If U be a non-empty open subset
of E∗
, such that the norm of all element in U are not zero, then theorem is
trivial. So assume that ϕ0 ∈ U, ϕ0 = 0 and define
U0 = {
1
ϕ0
ϕ : ϕ ∈ U}
Now we have
1
ϕ0
ϕ0 =
1
ϕ0
. ϕ0 = 1 ,
1
ϕ0
ϕ0 ∈ U0
So we have an open non-empty subset of E∗
contain an element of norm 1.
Now take δ > 0 such that,
U = {ϕ ∈ E∗
: ϕ < δ}
Specially, for 0 ∈ U we have 1 ∈ U, Now we just to proof that,
ϕn
∈ S , ∀n ≥ 0 , ∀ϕ ∈ U
For this, suppose that ϕn
∈ U for ϕn
∈ U and n ≤ k − 1. In this way we have
ψt =
etϕ
− 1 − tϕ − (tϕ)2
2!
− . . . − (tϕ)k
k!
tk
Since tϕ ∈ U, assume that x ∈ E be given, then
|(ψt −
ϕk
k!
)(x)| = |
1
tk
(etϕ
− 1 − tϕ −
(tϕ)2
2!
− . . . −
(tϕ)k
k!
)(x)|
running head 5
≤ t
n≥k+1
tn−k−1 |ϕ(x)|n
n!
≤ teδ x
Then in the space Hbc(E) we have
ψt →
ϕk
k!
, t → ∞
So ϕk
k!
∈ S, and by this the proof is complete.
Theorem 3.3 Let E is a banach space with dual E∗
and 0 = α ∈ E be Non-
constant member in H(C) of the exponential type φ(z) = ∞
n=0 Cnzn
, Then the
operator φα(D) : Hbc(E) → Hbc(E) defined by φα(D) = ∞
n=0 cnDnf(.)α is a
hypercyclic operator.
Proof. Let ψ : E∗ → C defined by ψ(ϕ) = ∞
n=0 Pn(ϕ), in which each
function Pn : E∗ → C be n-similar polynomials, such that for each n ≥ 0 are
defined by Pn(ϕ) = cnϕn(α). Now, since ϕ is the exponential type, so there is
R > 0 so that we have |cn| ≤ Rn
n!
for each n ≥ 0. Consider ϕ ∈ E∗ with the
condition ϕ ≤ 1, Now for n ≥ 0, we have
|Pn(ϕ)| = |cnϕn(α)| = |cn|.|ϕn(α)| ≤
Rn
n!
ϕ n
. α n
≤ (
c. α .R
n
)n
|Pn(ϕ)| ≤ (
c. α .R
n
)n
|Pn(ϕ)|1
n
≤ (
c. α .R
n
)
then
|Pn(ϕ)|
1
n → 0 , n → ∞
so ψ : E∗
→ C is entire, bounded and nonconstant. Since ψ : E∗
→ C is
nonconstant, then the sets
U = {ϕ ∈ E∗
: |
∞
n=0
Pn(ϕ)| = |ψ(ϕ)| < 1}
and
V = {ϕ ∈ E∗
: |
∞
n=0
Pn(ϕ)| = |ψ(ϕ)| > 1}
are open and non-empty, so by theorem2.2 two sets
X0 = Span{eϕ
: ϕ ∈ U} , Y0 = Span{eϕ
: ϕ ∈ V }
6 P. Karami, M. Habibi, F. Safari, M. Zarrabi
are dense subspaces of Hbc(E). If T = Φ(D) then
T(eϕ
) =
∞
0
cnDn(eϕ)α =
∞
0
cnϕn
(α)eϕ
= eϕ
∞
0
cnϕn
(α) = eϕ
ψ(ϕ)
by theorem2.
Tn
→ 0 , n → ∞ , pointwise on X0
Also by theorem2.1 we conclude that, there is a map S : Y0 → Y0 defined by
S(eϕ
) = |ψ(ϕ)|eϕ
such that,
Sn
→ 0 , n → ∞ , pointwise on Y0
and TS = IY
so by Kitai-Getner-Shapiro theorem the operator T = Φα(D) is hypercyclic
operator.
Corollary 3.4 If E be a Banach space with separable dual E∗
, then the
space Hbc(E) admitted a hypercyclic operator.(Also E∗
)
Corollary 3.5 Let E be a Banach space with separable dual E∗
and 0 =
α ∈ E, then operator Tα definition by Tαf(x) = f(x + α) on Hbc(E) is a
hypercyclic operator.
ACKNOWLEDGEMENTS. This research was partially supported by a
grant from Research Council of Islamic Azad University, Branch of Mamasani,
so the authors gratefully acknowledge this support.
References
[1] B. Beauzamy , An Operator on a Separable Hilbert Space with all Poly-
nomials Hypercyclic, Studia Math. Theory , XCVI, (1990), 81-90.
[2] L. Bernal-Gonzalez and A. Montes-Rodryguez, Non-finite Dimensional
closed vector Spaces of universal Functions for Composition Operators,
Jour. Approx. Theory ,82, (1995), 375-391.
[3] J. Bes, Invariant manifolds of hypercyclic vectors for the real scalar case,
Proc. Amer. Math. Soc. , 127 (1999), 1801-1804.
running head 7
[4] B. Bourdon, Invariant Manifolds of Hypercyclic Vectors, Proc. Amer.
Math. Soc. , 118 , No. 3 (1993), 845-847.
[5] P. R. Halmos, Measure Theory, Van Nostrand, New York, 1950.
[6] D. A. Herrero, Hypercyclic Operators and Chaos,Jour. of Op. Theory, 28
(1992), 93-103.
[7] C. Kitai, Invariant Closed Sets for Linear Operators ,Thesis, University
of Toronto (1982).
[8] F. Leon-Saavedra, Operators with Hypercyclic Cesaro Means, Studia
math. , 154, No. 3 (2002).
[9] J. Lindenstrauss and L. Tzafriri, Claccical Banach Spaces I, Springer-
Verlag, Heidelberg, 1977.
[10] G. R. MacLane, Sequences of derivatives and normal families, Jour. Anal.
Math., 2 (1952),72-87.
[11] A. Montes-Rodrguez, Banach Spaces of Hypercyclic vectors, Michigan
Math. Jour. ,43, No. 3 (1996), 419-436.
[12] J. H. Shapiro, Composition Operators and classical function theory,
Springer-Verlag, 1993.
Received: Month xx, 200x

More Related Content

What's hot

Congruence Lattices of A Finite Uniform Lattices
Congruence Lattices of A Finite Uniform LatticesCongruence Lattices of A Finite Uniform Lattices
Congruence Lattices of A Finite Uniform Latticesinventionjournals
 
differentiate free
differentiate freedifferentiate free
differentiate freelydmilaroy
 
11.[29 35]a unique common fixed point theorem under psi varphi contractive co...
11.[29 35]a unique common fixed point theorem under psi varphi contractive co...11.[29 35]a unique common fixed point theorem under psi varphi contractive co...
11.[29 35]a unique common fixed point theorem under psi varphi contractive co...Alexander Decker
 
(C f)- weak contraction in cone metric spaces
(C f)- weak contraction in cone metric spaces(C f)- weak contraction in cone metric spaces
(C f)- weak contraction in cone metric spacesAlexander Decker
 
Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)Matthew Leingang
 
Harmonic Analysis and Deep Learning
Harmonic Analysis and Deep LearningHarmonic Analysis and Deep Learning
Harmonic Analysis and Deep LearningSungbin Lim
 
2 polar graphs
2 polar graphs2 polar graphs
2 polar graphsmath267
 
Linear Programming
Linear ProgrammingLinear Programming
Linear Programmingknspavan
 
Herbrand-satisfiability of a Quantified Set-theoretical Fragment (Cantone, Lo...
Herbrand-satisfiability of a Quantified Set-theoretical Fragment (Cantone, Lo...Herbrand-satisfiability of a Quantified Set-theoretical Fragment (Cantone, Lo...
Herbrand-satisfiability of a Quantified Set-theoretical Fragment (Cantone, Lo...Cristiano Longo
 
Probability cheatsheet
Probability cheatsheetProbability cheatsheet
Probability cheatsheetSuvrat Mishra
 
Ian.petrow【transcendental number theory】.
Ian.petrow【transcendental number theory】.Ian.petrow【transcendental number theory】.
Ian.petrow【transcendental number theory】.Tong Leung
 
Numerical Fourier transform based on hyperfunction theory
Numerical Fourier transform based on hyperfunction theoryNumerical Fourier transform based on hyperfunction theory
Numerical Fourier transform based on hyperfunction theoryHidenoriOgata
 
Quantum optical models in noncommutative spaces
Quantum optical models in noncommutative spacesQuantum optical models in noncommutative spaces
Quantum optical models in noncommutative spacesSanjib Dey
 
Hyperfunction method for numerical integration and Fredholm integral equation...
Hyperfunction method for numerical integration and Fredholm integral equation...Hyperfunction method for numerical integration and Fredholm integral equation...
Hyperfunction method for numerical integration and Fredholm integral equation...HidenoriOgata
 
Cs229 notes8
Cs229 notes8Cs229 notes8
Cs229 notes8VuTran231
 
T--Pre –Operattors
T--Pre –OperattorsT--Pre –Operattors
T--Pre –OperattorsIOSR Journals
 

What's hot (20)

Congruence Lattices of A Finite Uniform Lattices
Congruence Lattices of A Finite Uniform LatticesCongruence Lattices of A Finite Uniform Lattices
Congruence Lattices of A Finite Uniform Lattices
 
differentiate free
differentiate freedifferentiate free
differentiate free
 
11.[29 35]a unique common fixed point theorem under psi varphi contractive co...
11.[29 35]a unique common fixed point theorem under psi varphi contractive co...11.[29 35]a unique common fixed point theorem under psi varphi contractive co...
11.[29 35]a unique common fixed point theorem under psi varphi contractive co...
 
(C f)- weak contraction in cone metric spaces
(C f)- weak contraction in cone metric spaces(C f)- weak contraction in cone metric spaces
(C f)- weak contraction in cone metric spaces
 
Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)
 
Harmonic Analysis and Deep Learning
Harmonic Analysis and Deep LearningHarmonic Analysis and Deep Learning
Harmonic Analysis and Deep Learning
 
2 polar graphs
2 polar graphs2 polar graphs
2 polar graphs
 
Linear Programming
Linear ProgrammingLinear Programming
Linear Programming
 
Herbrand-satisfiability of a Quantified Set-theoretical Fragment (Cantone, Lo...
Herbrand-satisfiability of a Quantified Set-theoretical Fragment (Cantone, Lo...Herbrand-satisfiability of a Quantified Set-theoretical Fragment (Cantone, Lo...
Herbrand-satisfiability of a Quantified Set-theoretical Fragment (Cantone, Lo...
 
Probability cheatsheet
Probability cheatsheetProbability cheatsheet
Probability cheatsheet
 
Matrix calculus
Matrix calculusMatrix calculus
Matrix calculus
 
Ch7
Ch7Ch7
Ch7
 
Ian.petrow【transcendental number theory】.
Ian.petrow【transcendental number theory】.Ian.petrow【transcendental number theory】.
Ian.petrow【transcendental number theory】.
 
Numerical Fourier transform based on hyperfunction theory
Numerical Fourier transform based on hyperfunction theoryNumerical Fourier transform based on hyperfunction theory
Numerical Fourier transform based on hyperfunction theory
 
Analysis Solutions CIV
Analysis Solutions CIVAnalysis Solutions CIV
Analysis Solutions CIV
 
Quantum optical models in noncommutative spaces
Quantum optical models in noncommutative spacesQuantum optical models in noncommutative spaces
Quantum optical models in noncommutative spaces
 
Hyperfunction method for numerical integration and Fredholm integral equation...
Hyperfunction method for numerical integration and Fredholm integral equation...Hyperfunction method for numerical integration and Fredholm integral equation...
Hyperfunction method for numerical integration and Fredholm integral equation...
 
BAYSM'14, Wien, Austria
BAYSM'14, Wien, AustriaBAYSM'14, Wien, Austria
BAYSM'14, Wien, Austria
 
Cs229 notes8
Cs229 notes8Cs229 notes8
Cs229 notes8
 
T--Pre –Operattors
T--Pre –OperattorsT--Pre –Operattors
T--Pre –Operattors
 

Viewers also liked

merged_document_entreschool
merged_document_entreschoolmerged_document_entreschool
merged_document_entreschoolKritika Parwal
 
PaperNo14-Habibi-IJMA-n-Tuples and Chaoticity
PaperNo14-Habibi-IJMA-n-Tuples and ChaoticityPaperNo14-Habibi-IJMA-n-Tuples and Chaoticity
PaperNo14-Habibi-IJMA-n-Tuples and ChaoticityMezban Habibi
 
PaperNo21-habibi-IJMTT-V8P514-IJMMT
PaperNo21-habibi-IJMTT-V8P514-IJMMTPaperNo21-habibi-IJMTT-V8P514-IJMMT
PaperNo21-habibi-IJMTT-V8P514-IJMMTMezban Habibi
 
Apostolul 178 - Iunie 2015
Apostolul 178 - Iunie 2015Apostolul 178 - Iunie 2015
Apostolul 178 - Iunie 2015SCOLI MUSATINE
 
Lexgenda Documenti d’archivio e nuove tecnologie
Lexgenda Documenti d’archivio e nuove tecnologieLexgenda Documenti d’archivio e nuove tecnologie
Lexgenda Documenti d’archivio e nuove tecnologieNicola Del Gobbo
 
PaperNo19-habibiIJMA13-16-2013-IJMA
PaperNo19-habibiIJMA13-16-2013-IJMAPaperNo19-habibiIJMA13-16-2013-IJMA
PaperNo19-habibiIJMA13-16-2013-IJMAMezban Habibi
 

Viewers also liked (13)

merged_document_entreschool
merged_document_entreschoolmerged_document_entreschool
merged_document_entreschool
 
Youth section
Youth sectionYouth section
Youth section
 
PaperNo14-Habibi-IJMA-n-Tuples and Chaoticity
PaperNo14-Habibi-IJMA-n-Tuples and ChaoticityPaperNo14-Habibi-IJMA-n-Tuples and Chaoticity
PaperNo14-Habibi-IJMA-n-Tuples and Chaoticity
 
PaperNo21-habibi-IJMTT-V8P514-IJMMT
PaperNo21-habibi-IJMTT-V8P514-IJMMTPaperNo21-habibi-IJMTT-V8P514-IJMMT
PaperNo21-habibi-IJMTT-V8P514-IJMMT
 
diss_vanderwulp2015
diss_vanderwulp2015diss_vanderwulp2015
diss_vanderwulp2015
 
Apostolul 178 - Iunie 2015
Apostolul 178 - Iunie 2015Apostolul 178 - Iunie 2015
Apostolul 178 - Iunie 2015
 
For body
For bodyFor body
For body
 
Lexgenda Documenti d’archivio e nuove tecnologie
Lexgenda Documenti d’archivio e nuove tecnologieLexgenda Documenti d’archivio e nuove tecnologie
Lexgenda Documenti d’archivio e nuove tecnologie
 
Skin care
Skin careSkin care
Skin care
 
VVD-Banner-85x200cm-V1
VVD-Banner-85x200cm-V1VVD-Banner-85x200cm-V1
VVD-Banner-85x200cm-V1
 
PaperNo19-habibiIJMA13-16-2013-IJMA
PaperNo19-habibiIJMA13-16-2013-IJMAPaperNo19-habibiIJMA13-16-2013-IJMA
PaperNo19-habibiIJMA13-16-2013-IJMA
 
G460
G460G460
G460
 
The me of Things
The me of ThingsThe me of Things
The me of Things
 

Similar to PaperNo10-KaramiHabibiSafariZarrabi-IJCMS

Approximation Methods Of Solutions For Equilibrium Problem In Hilbert Spaces
Approximation Methods Of Solutions For Equilibrium Problem In Hilbert SpacesApproximation Methods Of Solutions For Equilibrium Problem In Hilbert Spaces
Approximation Methods Of Solutions For Equilibrium Problem In Hilbert SpacesLisa Garcia
 
Functionalanalysis ejemplos infinitos
Functionalanalysis ejemplos infinitosFunctionalanalysis ejemplos infinitos
Functionalanalysis ejemplos infinitosSualín Rojas
 
Measure Theory and important points with booklet
Measure Theory and important points with bookletMeasure Theory and important points with booklet
Measure Theory and important points with bookletNaeemAhmad289736
 
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...IOSR Journals
 
Fixed Point Results In Fuzzy Menger Space With Common Property (E.A.)
Fixed Point Results In Fuzzy Menger Space With Common Property (E.A.)Fixed Point Results In Fuzzy Menger Space With Common Property (E.A.)
Fixed Point Results In Fuzzy Menger Space With Common Property (E.A.)IJERA Editor
 
Real Analysis II (Measure Theory) Notes
Real Analysis II (Measure Theory) NotesReal Analysis II (Measure Theory) Notes
Real Analysis II (Measure Theory) NotesPrakash Dabhi
 
Limit in Dual Space
Limit in Dual SpaceLimit in Dual Space
Limit in Dual SpaceQUESTJOURNAL
 
International Journal of Mathematics and Statistics Invention (IJMSI)
International Journal of Mathematics and Statistics Invention (IJMSI) International Journal of Mathematics and Statistics Invention (IJMSI)
International Journal of Mathematics and Statistics Invention (IJMSI) inventionjournals
 
On Frechet Derivatives with Application to the Inverse Function Theorem of Or...
On Frechet Derivatives with Application to the Inverse Function Theorem of Or...On Frechet Derivatives with Application to the Inverse Function Theorem of Or...
On Frechet Derivatives with Application to the Inverse Function Theorem of Or...BRNSS Publication Hub
 
A Komlo ́sTheorem for general Banach lattices of measurable functions
A Komlo ́sTheorem for general Banach lattices of measurable functionsA Komlo ́sTheorem for general Banach lattices of measurable functions
A Komlo ́sTheorem for general Banach lattices of measurable functionsesasancpe
 
PaperNo1-ErshadYousefiHabibi-IJMS
PaperNo1-ErshadYousefiHabibi-IJMSPaperNo1-ErshadYousefiHabibi-IJMS
PaperNo1-ErshadYousefiHabibi-IJMSMezban Habibi
 
On Extendable Sets in the Reals (R) With Application to the Lyapunov Stabilit...
On Extendable Sets in the Reals (R) With Application to the Lyapunov Stabilit...On Extendable Sets in the Reals (R) With Application to the Lyapunov Stabilit...
On Extendable Sets in the Reals (R) With Application to the Lyapunov Stabilit...BRNSS Publication Hub
 
Measure and integration
Measure and integrationMeasure and integration
Measure and integrationPrakash Dabhi
 

Similar to PaperNo10-KaramiHabibiSafariZarrabi-IJCMS (20)

Approximation Methods Of Solutions For Equilibrium Problem In Hilbert Spaces
Approximation Methods Of Solutions For Equilibrium Problem In Hilbert SpacesApproximation Methods Of Solutions For Equilibrium Problem In Hilbert Spaces
Approximation Methods Of Solutions For Equilibrium Problem In Hilbert Spaces
 
math camp
math campmath camp
math camp
 
Functionalanalysis ejemplos infinitos
Functionalanalysis ejemplos infinitosFunctionalanalysis ejemplos infinitos
Functionalanalysis ejemplos infinitos
 
Measure Theory and important points with booklet
Measure Theory and important points with bookletMeasure Theory and important points with booklet
Measure Theory and important points with booklet
 
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
 
project
projectproject
project
 
Fixed Point Results In Fuzzy Menger Space With Common Property (E.A.)
Fixed Point Results In Fuzzy Menger Space With Common Property (E.A.)Fixed Point Results In Fuzzy Menger Space With Common Property (E.A.)
Fixed Point Results In Fuzzy Menger Space With Common Property (E.A.)
 
Imc2017 day2-solutions
Imc2017 day2-solutionsImc2017 day2-solutions
Imc2017 day2-solutions
 
Real Analysis II (Measure Theory) Notes
Real Analysis II (Measure Theory) NotesReal Analysis II (Measure Theory) Notes
Real Analysis II (Measure Theory) Notes
 
Limit in Dual Space
Limit in Dual SpaceLimit in Dual Space
Limit in Dual Space
 
International Journal of Mathematics and Statistics Invention (IJMSI)
International Journal of Mathematics and Statistics Invention (IJMSI) International Journal of Mathematics and Statistics Invention (IJMSI)
International Journal of Mathematics and Statistics Invention (IJMSI)
 
05_AJMS_300_21.pdf
05_AJMS_300_21.pdf05_AJMS_300_21.pdf
05_AJMS_300_21.pdf
 
On Frechet Derivatives with Application to the Inverse Function Theorem of Or...
On Frechet Derivatives with Application to the Inverse Function Theorem of Or...On Frechet Derivatives with Application to the Inverse Function Theorem of Or...
On Frechet Derivatives with Application to the Inverse Function Theorem of Or...
 
A Komlo ́sTheorem for general Banach lattices of measurable functions
A Komlo ́sTheorem for general Banach lattices of measurable functionsA Komlo ́sTheorem for general Banach lattices of measurable functions
A Komlo ́sTheorem for general Banach lattices of measurable functions
 
PaperNo1-ErshadYousefiHabibi-IJMS
PaperNo1-ErshadYousefiHabibi-IJMSPaperNo1-ErshadYousefiHabibi-IJMS
PaperNo1-ErshadYousefiHabibi-IJMS
 
1_AJMS_229_19[Review].pdf
1_AJMS_229_19[Review].pdf1_AJMS_229_19[Review].pdf
1_AJMS_229_19[Review].pdf
 
Puy chosuantai2
Puy chosuantai2Puy chosuantai2
Puy chosuantai2
 
On Extendable Sets in the Reals (R) With Application to the Lyapunov Stabilit...
On Extendable Sets in the Reals (R) With Application to the Lyapunov Stabilit...On Extendable Sets in the Reals (R) With Application to the Lyapunov Stabilit...
On Extendable Sets in the Reals (R) With Application to the Lyapunov Stabilit...
 
Pata contraction
Pata contractionPata contraction
Pata contraction
 
Measure and integration
Measure and integrationMeasure and integration
Measure and integration
 

More from Mezban Habibi

PaperNo23-habibiIJCMS5-8-2014-IJCMS
PaperNo23-habibiIJCMS5-8-2014-IJCMSPaperNo23-habibiIJCMS5-8-2014-IJCMS
PaperNo23-habibiIJCMS5-8-2014-IJCMSMezban Habibi
 
PaperNo22-habibiIJMA17-20-2014-IJMA
PaperNo22-habibiIJMA17-20-2014-IJMAPaperNo22-habibiIJMA17-20-2014-IJMA
PaperNo22-habibiIJMA17-20-2014-IJMAMezban Habibi
 
PaperNo20-hoseinihabibiPMS1-4-2014-PMS
PaperNo20-hoseinihabibiPMS1-4-2014-PMSPaperNo20-hoseinihabibiPMS1-4-2014-PMS
PaperNo20-hoseinihabibiPMS1-4-2014-PMSMezban Habibi
 
PaperNo17-HabibiMasoudiSafari-IJCMA
PaperNo17-HabibiMasoudiSafari-IJCMAPaperNo17-HabibiMasoudiSafari-IJCMA
PaperNo17-HabibiMasoudiSafari-IJCMAMezban Habibi
 
PaperNo16-Habibi-IMF-On Syndetically Hypercyclic Tuples
PaperNo16-Habibi-IMF-On Syndetically Hypercyclic TuplesPaperNo16-Habibi-IMF-On Syndetically Hypercyclic Tuples
PaperNo16-Habibi-IMF-On Syndetically Hypercyclic TuplesMezban Habibi
 
PaperNo15-HoseiniHabibiSafariGhezelbash-IJMA
PaperNo15-HoseiniHabibiSafariGhezelbash-IJMAPaperNo15-HoseiniHabibiSafariGhezelbash-IJMA
PaperNo15-HoseiniHabibiSafariGhezelbash-IJMAMezban Habibi
 
PaperNo13-Habibi-IMF
PaperNo13-Habibi-IMFPaperNo13-Habibi-IMF
PaperNo13-Habibi-IMFMezban Habibi
 
PaperNo12-YousefiHabibi-IJAM
PaperNo12-YousefiHabibi-IJAMPaperNo12-YousefiHabibi-IJAM
PaperNo12-YousefiHabibi-IJAMMezban Habibi
 
PaperNo11-GHEZELBASHHABIBISAFARI-IJMMS
PaperNo11-GHEZELBASHHABIBISAFARI-IJMMSPaperNo11-GHEZELBASHHABIBISAFARI-IJMMS
PaperNo11-GHEZELBASHHABIBISAFARI-IJMMSMezban Habibi
 
PaperNo9-OSTADHABIBISAFARI-FJMS
PaperNo9-OSTADHABIBISAFARI-FJMSPaperNo9-OSTADHABIBISAFARI-FJMS
PaperNo9-OSTADHABIBISAFARI-FJMSMezban Habibi
 
PaperNo8-HabibiSafari-IJAM-CHAOTICITY OF A PAIR OF OPERATORS
PaperNo8-HabibiSafari-IJAM-CHAOTICITY OF A PAIR OF OPERATORSPaperNo8-HabibiSafari-IJAM-CHAOTICITY OF A PAIR OF OPERATORS
PaperNo8-HabibiSafari-IJAM-CHAOTICITY OF A PAIR OF OPERATORSMezban Habibi
 
PaperNo7-YousefiHabibi-IJAM
PaperNo7-YousefiHabibi-IJAMPaperNo7-YousefiHabibi-IJAM
PaperNo7-YousefiHabibi-IJAMMezban Habibi
 
PaperNo5-HabibiYousefi-IJAM
PaperNo5-HabibiYousefi-IJAMPaperNo5-HabibiYousefi-IJAM
PaperNo5-HabibiYousefi-IJAMMezban Habibi
 
PaperNo6-YousefiHabibi-IJAM
PaperNo6-YousefiHabibi-IJAMPaperNo6-YousefiHabibi-IJAM
PaperNo6-YousefiHabibi-IJAMMezban Habibi
 
PaperNo4-HABIBISAFARI-FJMS
PaperNo4-HABIBISAFARI-FJMSPaperNo4-HABIBISAFARI-FJMS
PaperNo4-HABIBISAFARI-FJMSMezban Habibi
 
PaperNo3-YousefiHabibi-IMF
PaperNo3-YousefiHabibi-IMFPaperNo3-YousefiHabibi-IMF
PaperNo3-YousefiHabibi-IMFMezban Habibi
 

More from Mezban Habibi (20)

Record B.S.
Record B.S.Record B.S.
Record B.S.
 
T.T.
T.T.T.T.
T.T.
 
B.S.
B.S.B.S.
B.S.
 
M.S.
M.S.M.S.
M.S.
 
PaperNo23-habibiIJCMS5-8-2014-IJCMS
PaperNo23-habibiIJCMS5-8-2014-IJCMSPaperNo23-habibiIJCMS5-8-2014-IJCMS
PaperNo23-habibiIJCMS5-8-2014-IJCMS
 
PaperNo22-habibiIJMA17-20-2014-IJMA
PaperNo22-habibiIJMA17-20-2014-IJMAPaperNo22-habibiIJMA17-20-2014-IJMA
PaperNo22-habibiIJMA17-20-2014-IJMA
 
PaperNo20-hoseinihabibiPMS1-4-2014-PMS
PaperNo20-hoseinihabibiPMS1-4-2014-PMSPaperNo20-hoseinihabibiPMS1-4-2014-PMS
PaperNo20-hoseinihabibiPMS1-4-2014-PMS
 
PaperNo17-HabibiMasoudiSafari-IJCMA
PaperNo17-HabibiMasoudiSafari-IJCMAPaperNo17-HabibiMasoudiSafari-IJCMA
PaperNo17-HabibiMasoudiSafari-IJCMA
 
PaperNo16-Habibi-IMF-On Syndetically Hypercyclic Tuples
PaperNo16-Habibi-IMF-On Syndetically Hypercyclic TuplesPaperNo16-Habibi-IMF-On Syndetically Hypercyclic Tuples
PaperNo16-Habibi-IMF-On Syndetically Hypercyclic Tuples
 
PaperNo15-HoseiniHabibiSafariGhezelbash-IJMA
PaperNo15-HoseiniHabibiSafariGhezelbash-IJMAPaperNo15-HoseiniHabibiSafariGhezelbash-IJMA
PaperNo15-HoseiniHabibiSafariGhezelbash-IJMA
 
PaperNo13-Habibi-IMF
PaperNo13-Habibi-IMFPaperNo13-Habibi-IMF
PaperNo13-Habibi-IMF
 
PaperNo12-YousefiHabibi-IJAM
PaperNo12-YousefiHabibi-IJAMPaperNo12-YousefiHabibi-IJAM
PaperNo12-YousefiHabibi-IJAM
 
PaperNo11-GHEZELBASHHABIBISAFARI-IJMMS
PaperNo11-GHEZELBASHHABIBISAFARI-IJMMSPaperNo11-GHEZELBASHHABIBISAFARI-IJMMS
PaperNo11-GHEZELBASHHABIBISAFARI-IJMMS
 
PaperNo9-OSTADHABIBISAFARI-FJMS
PaperNo9-OSTADHABIBISAFARI-FJMSPaperNo9-OSTADHABIBISAFARI-FJMS
PaperNo9-OSTADHABIBISAFARI-FJMS
 
PaperNo8-HabibiSafari-IJAM-CHAOTICITY OF A PAIR OF OPERATORS
PaperNo8-HabibiSafari-IJAM-CHAOTICITY OF A PAIR OF OPERATORSPaperNo8-HabibiSafari-IJAM-CHAOTICITY OF A PAIR OF OPERATORS
PaperNo8-HabibiSafari-IJAM-CHAOTICITY OF A PAIR OF OPERATORS
 
PaperNo7-YousefiHabibi-IJAM
PaperNo7-YousefiHabibi-IJAMPaperNo7-YousefiHabibi-IJAM
PaperNo7-YousefiHabibi-IJAM
 
PaperNo5-HabibiYousefi-IJAM
PaperNo5-HabibiYousefi-IJAMPaperNo5-HabibiYousefi-IJAM
PaperNo5-HabibiYousefi-IJAM
 
PaperNo6-YousefiHabibi-IJAM
PaperNo6-YousefiHabibi-IJAMPaperNo6-YousefiHabibi-IJAM
PaperNo6-YousefiHabibi-IJAM
 
PaperNo4-HABIBISAFARI-FJMS
PaperNo4-HABIBISAFARI-FJMSPaperNo4-HABIBISAFARI-FJMS
PaperNo4-HABIBISAFARI-FJMS
 
PaperNo3-YousefiHabibi-IMF
PaperNo3-YousefiHabibi-IMFPaperNo3-YousefiHabibi-IMF
PaperNo3-YousefiHabibi-IMF
 

PaperNo10-KaramiHabibiSafariZarrabi-IJCMS

  • 1. Int. J. Contemp. Math. Sciences, Vol. 6, 2011, no. 36, 1761 - 1767 DENSITY AND INDEPENDENTLY ON Hbc(E) Parvin Karami department of mathematics Islamic Azad University, branch of Mamasani P.O.Box ..., Mamasani, Iran karami-pk67@yahoo.com Mezban Habibi department of mathematics Islamic Azad University, branch of Mamasani P.O.Box ..., Mamasani, Iran habibi.m@iaudehdasht.ac.ir Fatemeh Safari department of mathematics Islamic Azad University, branch of Mamasani P.O.Box ..., Mamasani, Iran safari.s@iaudehdasht.ac.ir Mohammad Zarrabi department of mathematics Islamic Azad University, branch of Mamasani P.O.Box ..., Mamasani, Iran m-zarrabi86@yahoo.com Abstract The aim of the paper ahead Birhoff , Maclane, Godefroy-Shapiro and Kitai-Getner-Shapiro and the results of their theorems and hypercyclic operators on space H(C). In Birhoffs theorem is shown that, if b is non-zero, then the shift with the vector b is an hypercyclic operator. Maclane in 1952 showed that the Differentiation operator on H(C) is an hypercyclic operator. Bourdon and Shapiro also studied the behavior of operators composition operaotrs on this space. For more information reader can see [1–14].
  • 2. 2 P. Karami, M. Habibi, F. Safari, M. Zarrabi Subject Classification: 47A16,47B37 Keywords:Hypercyclic vector, Hypercyclicity criterion, Differentiation op- erator, Density, Independently, Dual space. 1 Introduction Let X be a frechet space and T be bounded linear operators on X. For each x ∈ X put Orb(T, x) = {Tn (x) : n ≥ 0)} = {x, Tx, T2 x, T3 x, . . .} The set Orb(T, x) is called orbit of vector x under the operator T and the operator T is called hypercyclic operator if there exist vector x in X such that the set Orb(T, x) is dense in X, that is Orb(T, x) = {x, Tx, T2x, T3x, . . .} = X. In this case a vector x is called hypercyclic vector for the operator. If X∗ be the dual of space X and both operators T : X → X and T∗ : X∗ → X∗ are hypercyclic, then the operator T is called dual hypercyclic.(Note that if X be a bounded space, then the dual of X denoted by X ). If M is a subset of X and all non-zero element of space M be a hpercyclic vector for T, then M is called hypercyclic subspace of X. 2 Preliminary Notes Suppose that H(C) be the space of all functions of one complex variable with the uniform convergence topology on compact subsets of C. Consider Banach space E, Ferechet algebra by elements of dual space with uniform convergence topology over the balls of E. Space Hbc(E) containing all bounded functions on compact subsets of E, the space Hbc(E) includes all functions f = ∞ n=0 Pn in which Pn ∈ Span{ϕn : ϕE∗} , n = 0, 1, 2, 3, ... Pn 1 n = (Sup x <1|Pn|) 1 n → 0 , n → ∞ The operator φ : H(E) → H(E) by definition φ(f) = Df is called differen- tiation operator. Let ϕ ∈ H(C), then the operator Cϕ : H(C) → H(C) by definition Cϕ(f) = foϕ on H(C) is hypercyclic, if and only if the operator ϕ is a shift with a non-zero vector b ∈ C. In other words, ∃0 = b ∈ C, ϕ(z) = z+b(see[1]). Differentiation operator on H(C) is a hypercyclic operator(see[6]).
  • 3. running head 3 If φ(z) = |α|≥0 Cαzα be non-constant entire function on C, Then the oper- ator φD : H(Cn ) → H(Cn ) by definition φD(f) = |α|≥0 CαDα f, f ∈ H(C) is hypercyclic operator(see[10]). Also all continuous linear operator on H(Cn ) substitute with translation, if and only if, be for one ϕ ∈ H(Cn ) is of expo- nential form T = ϕ D (see[10]). Let X be an F-space and T : X → X be a continuous linear operator and assume that X0, Y0 are two dense subsets of X and {nk}∞ k=1 be a sequence of positive integers, and there are sequences Snk : Y0 → X of mapping such that, (1). Tnk → 0, k → ∞ , Pointwise on X0 (2). Snk → 0, k → ∞ , Pointwise on Y0 (3). Tnk Snk = IY0 then the operator T is hypercyclic(Hypercyclic Creterion) 3 Main Results Theorem 3.1 The collection B = {eϕ : ϕ ∈ E∗ } is a independently linear subset of Hbc(E). Proof. Let {eϕi }i∈I be the maximal independently linear subset of B. Sup- pose ϕ ∈ E∗ be fix point, and ζi1 , ζi2 , ..., ζir ∈ C with the condition, ζi1 .eϕi1 + ζi2 .eϕi2 + . . . + ζir .eϕir = eϕ Let α be a trivial element of E. Use the Operator f → df(.)α in bellow equation, we have, df(ζi1 .eϕi1 + ζi2 .eϕi2 + . . . + ζir .eϕir )(α) = df(eϕ ) so df(ζi1 .eϕi1 )(α) + df(ζi2 .eϕi2 )(α) + . . . + df(ζir .eϕir )(α) = df(eϕ )(α) ζi1 .ϕi1 (α).eϕi1 + ζi2 .ϕi2 (α).eϕi2 + . . . + ζir .ϕir (α).eϕir = ϕ(α).eϕ Since {eϕi }i∈I is a independently linear subset of B and ζi1 , ζi2 , ..., ζir ∈ C are non-zero elements, then ϕi1 (α) = ϕi2 (α) = . . . = ϕir (α) Now, since α be a trivial element of E, then ϕi1 = ϕi2 = . . . = ϕir So {eϕi }i∈I = C∗ , by this the proof is complete.
  • 4. 4 P. Karami, M. Habibi, F. Safari, M. Zarrabi Theorem 3.2 Let U be an open subset of E∗ , then S = Span{eϕ : ϕ ∈ U} is a dense subset of Hbc(E). Proof. Let ϕ0 ∈ E∗ and Λ : Hbc(E) → Hbc(E) bye Λ(ψ) = eϕ0 .ψ. Suppose ψ1, ψ2 ∈ Hbc(E) and Λ(ψ)1 = Λ(ψ)2, so eϕ0 .ψ1 = eϕ0 .ψ2. Since eϕ0 = 0, then ψ1 = ψ2, that is the operator Λ is one-one operator. Since constant opera- tor and identity operator are continuous, then the operator Λ is continuous. Now since Λ(ψ)−1 = e−ϕ0 .ψ is continuous operator, then the operator Λ is a homeomorphism and Span{eϕ0+ϕ : ϕ ∈ U} = Hbc(E) ⇔ Span{e+ϕ : ϕ ∈ U} = Hbc(E) If λo ∈ U then take U0 = {ϕ − λ0 : ϕ ∈ U}, then 0 = λ0 − λ0 ∈ U0, So without lost of generality we can suppose 0 ∈ U. If U be a non-empty open subset of E∗ , such that the norm of all element in U are not zero, then theorem is trivial. So assume that ϕ0 ∈ U, ϕ0 = 0 and define U0 = { 1 ϕ0 ϕ : ϕ ∈ U} Now we have 1 ϕ0 ϕ0 = 1 ϕ0 . ϕ0 = 1 , 1 ϕ0 ϕ0 ∈ U0 So we have an open non-empty subset of E∗ contain an element of norm 1. Now take δ > 0 such that, U = {ϕ ∈ E∗ : ϕ < δ} Specially, for 0 ∈ U we have 1 ∈ U, Now we just to proof that, ϕn ∈ S , ∀n ≥ 0 , ∀ϕ ∈ U For this, suppose that ϕn ∈ U for ϕn ∈ U and n ≤ k − 1. In this way we have ψt = etϕ − 1 − tϕ − (tϕ)2 2! − . . . − (tϕ)k k! tk Since tϕ ∈ U, assume that x ∈ E be given, then |(ψt − ϕk k! )(x)| = | 1 tk (etϕ − 1 − tϕ − (tϕ)2 2! − . . . − (tϕ)k k! )(x)|
  • 5. running head 5 ≤ t n≥k+1 tn−k−1 |ϕ(x)|n n! ≤ teδ x Then in the space Hbc(E) we have ψt → ϕk k! , t → ∞ So ϕk k! ∈ S, and by this the proof is complete. Theorem 3.3 Let E is a banach space with dual E∗ and 0 = α ∈ E be Non- constant member in H(C) of the exponential type φ(z) = ∞ n=0 Cnzn , Then the operator φα(D) : Hbc(E) → Hbc(E) defined by φα(D) = ∞ n=0 cnDnf(.)α is a hypercyclic operator. Proof. Let ψ : E∗ → C defined by ψ(ϕ) = ∞ n=0 Pn(ϕ), in which each function Pn : E∗ → C be n-similar polynomials, such that for each n ≥ 0 are defined by Pn(ϕ) = cnϕn(α). Now, since ϕ is the exponential type, so there is R > 0 so that we have |cn| ≤ Rn n! for each n ≥ 0. Consider ϕ ∈ E∗ with the condition ϕ ≤ 1, Now for n ≥ 0, we have |Pn(ϕ)| = |cnϕn(α)| = |cn|.|ϕn(α)| ≤ Rn n! ϕ n . α n ≤ ( c. α .R n )n |Pn(ϕ)| ≤ ( c. α .R n )n |Pn(ϕ)|1 n ≤ ( c. α .R n ) then |Pn(ϕ)| 1 n → 0 , n → ∞ so ψ : E∗ → C is entire, bounded and nonconstant. Since ψ : E∗ → C is nonconstant, then the sets U = {ϕ ∈ E∗ : | ∞ n=0 Pn(ϕ)| = |ψ(ϕ)| < 1} and V = {ϕ ∈ E∗ : | ∞ n=0 Pn(ϕ)| = |ψ(ϕ)| > 1} are open and non-empty, so by theorem2.2 two sets X0 = Span{eϕ : ϕ ∈ U} , Y0 = Span{eϕ : ϕ ∈ V }
  • 6. 6 P. Karami, M. Habibi, F. Safari, M. Zarrabi are dense subspaces of Hbc(E). If T = Φ(D) then T(eϕ ) = ∞ 0 cnDn(eϕ)α = ∞ 0 cnϕn (α)eϕ = eϕ ∞ 0 cnϕn (α) = eϕ ψ(ϕ) by theorem2. Tn → 0 , n → ∞ , pointwise on X0 Also by theorem2.1 we conclude that, there is a map S : Y0 → Y0 defined by S(eϕ ) = |ψ(ϕ)|eϕ such that, Sn → 0 , n → ∞ , pointwise on Y0 and TS = IY so by Kitai-Getner-Shapiro theorem the operator T = Φα(D) is hypercyclic operator. Corollary 3.4 If E be a Banach space with separable dual E∗ , then the space Hbc(E) admitted a hypercyclic operator.(Also E∗ ) Corollary 3.5 Let E be a Banach space with separable dual E∗ and 0 = α ∈ E, then operator Tα definition by Tαf(x) = f(x + α) on Hbc(E) is a hypercyclic operator. ACKNOWLEDGEMENTS. This research was partially supported by a grant from Research Council of Islamic Azad University, Branch of Mamasani, so the authors gratefully acknowledge this support. References [1] B. Beauzamy , An Operator on a Separable Hilbert Space with all Poly- nomials Hypercyclic, Studia Math. Theory , XCVI, (1990), 81-90. [2] L. Bernal-Gonzalez and A. Montes-Rodryguez, Non-finite Dimensional closed vector Spaces of universal Functions for Composition Operators, Jour. Approx. Theory ,82, (1995), 375-391. [3] J. Bes, Invariant manifolds of hypercyclic vectors for the real scalar case, Proc. Amer. Math. Soc. , 127 (1999), 1801-1804.
  • 7. running head 7 [4] B. Bourdon, Invariant Manifolds of Hypercyclic Vectors, Proc. Amer. Math. Soc. , 118 , No. 3 (1993), 845-847. [5] P. R. Halmos, Measure Theory, Van Nostrand, New York, 1950. [6] D. A. Herrero, Hypercyclic Operators and Chaos,Jour. of Op. Theory, 28 (1992), 93-103. [7] C. Kitai, Invariant Closed Sets for Linear Operators ,Thesis, University of Toronto (1982). [8] F. Leon-Saavedra, Operators with Hypercyclic Cesaro Means, Studia math. , 154, No. 3 (2002). [9] J. Lindenstrauss and L. Tzafriri, Claccical Banach Spaces I, Springer- Verlag, Heidelberg, 1977. [10] G. R. MacLane, Sequences of derivatives and normal families, Jour. Anal. Math., 2 (1952),72-87. [11] A. Montes-Rodrguez, Banach Spaces of Hypercyclic vectors, Michigan Math. Jour. ,43, No. 3 (1996), 419-436. [12] J. H. Shapiro, Composition Operators and classical function theory, Springer-Verlag, 1993. Received: Month xx, 200x