Volume 2012, Article ID 729235,7pages doi:10.1155/2012/729235
Research Article
On Generalized Approximative
Properties of Systems
Turab Mursal Ahmedov and Zahira Vahid Mamedova
Institute of Mathematics and Mechanics, National Academy of Sciences of Azerbaijan, 9 B. Vaxabzade, Baku AZ1141, Azerbaijan
Correspondence should be addressed to Zahira Vahid Mamedova,zahira eng13@hotmail.com
Received 5 January 2012; Accepted 15 February 2012
Academic Editor: Siegfried Gottwald
Copyrightq2012 T. Mursal Ahmedov and Z. Vahid Mamedova. This is an open access article
distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Generalized concepts of b-completeness, b-independence, b-minimality, and b-basicity are
introduced. Corresponding concept of a space of coefficients is defined, and some of its properties
are stated.
1. Introduction
Theory of classical basisincluding Schauder basisis sufficiently well developed, and quite a good number of monographs such as Day1, Singer2, 3, Young 4, Bilalov, Veliyev
5, Ch. Heil6, and so forth have been dedicated to it so far. There are different versions and generalizations of the concept of classical basisfor more details see2,3. One of such generalizations is proposed in 5, 7. In these works, the concept of bY-invariance is first
introduced and then used to obtain main results. It should be noted that the condition of
bY-invariance implies the fact that the corresponding mapping is tensorial.
In our work, we neglect thebY-invariance condition. We give more detailed
consider-ation to the space of coefficients. We also state a criterion of basicity.
2. Needful Notations and Concepts
Let X, Y, Z be some Banach spaces, and let · X, · Y, · Z be the corresponding norms. Assume that we are given some bounded bilinear mappingb : X ×Y → Z, that is,bx;yZ ≤cxXyY, for allx∈X, for ally∈Y, wherecis an absolute constant. For simplicity, we denotexy≡ bx;y. LetM⊂Y be some set. ByLbMwe denote theb-span
ofM. So, by definition,LbM≡ {z∈Z:∃{xk}n1 ⊂X,∃{yk}n1 ⊂M, z
n
k1xkyk}. By·we
System{yn}n∈N⊂Yis calledb-linearly independent if∞n1xnyn0 inZimplies that
xn0,for alln∈N.
In the context of the above mentioned, the concept of usual completeness is stated as follows.
Definition 2.1. System{yn}n∈N⊂Y is calledb-complete inZifLb{yn}n∈N ≡Z. We will also
need the concepts ofb-biorthogonal system andb-basis.
Definition 2.2. System{yn∗}n∈N⊂LZ;Xis calledb-biorthogonal to the system{yn}n∈N⊂Y if
y∗
nxyk δnkx, for alln, k∈N, for allx∈X, whereδnkis the Kronecker symbol.
Definition 2.3. System{yn}n∈N ⊂ Y is calledb-basis inZif for for allz ∈ Z,∃!{xn}n∈N ⊂ X :
z∞n1xnyn.
To obtain our main results we will use the following concept.
Definition 2.4. System{yn}n∈N⊂Y is called nondegenerate if∃cn>0 : xX ≤cnxynZ, for
allx∈X, for alln∈N.
3. Main Results
3.1. Space of Coefficients
Let{yn}n∈N⊂Y be some system. Assume that
Ky≡
{xn}n∈N ⊂X: the series
∞
n1
xnyn converges inZ
. 3.1
With regard to the ordinary operations of addition and multiplication by a complex number,
Kyis a linear space. We introduce a norm · Ky inKyas follows:
xKy sup
m
m
n1
xnyn
Z
, 3.2
wherex≡ {xn}n∈N∈ Ky. In fact, it is clear that
λ xKy |λ| xKy, ∀λ∈C;
x1 x2Ky ≤ x1Ky x2Ky, ∀xk∈ Ky, k1,2.
3.3
Assume thatxKy 0 for somex ≡ {xn}n∈N ∈ Ky .Letn0 inf{n : xk 0, for allk ≤
n−1}. In what follows we will suppose that the system{yn}n∈Nis nondegenerate. Letn0< ∞.
We have
sup
m
m
n1
xnyn
Z
≥n0
n1
xnyn
Z
xn0yn0Z≥
1
But this is contrary toxKy 0. Consequently,n0 ∞, that is,x 0. Thus,Ky; · Ky
is a normed space. Let us show that it is complete. Let{xn}n∈N ⊂ Kybe some fundamental
sequence withxn≡ {xkn}k∈N⊂X. For arbitrary fixed numberk∈N. We have
xkn−xkn p
X≤ck
xkn−xkn pyk
Z ck k i1
xin−xin pyi− k−1
i1
xin−xin pyi
Z
≤2cksup
m m i1
xin−xin pyi
2ckxn−xn pKy −→0, asn, p−→ ∞.
3.5
As a result, for all fixed k ∈ N the sequence {xkn}n∈N is fundamental in X. Let xkn → xk, n → ∞. Let us take arbitrary positive ε. Then ∃n0: for all n ≥ n0, for all p ∈ N, we
havexn−xn pKy < ε. Thus
m k1
xkn−xkn pyk
Z
< ε, ∀n≥n0, ∀p, m∈N. 3.6
Passing to the limit asp → ∞yields
m k1
xkn−xk
yk Z
≤ε, ∀n≥n0, ∀m∈N. 3.7
It is easy to see that
mp
km
xkn−xk
yk Z
≤2ε, ∀n≥n0, ∀m, p∈N. 3.8
Since the series∞k1xknykconverges inZ, it is clear that∃m0n: for allm≥m
n
0 , for allp∈N,
we have
mp
km
xknyk
Z
< ε. 3.9
Then it follows from the previous inequality that
mkmpxkyk
Z
≤ mp
km
xkn−xk
yk Z
mp
km
xknyk
Z
≤ 3ε,
∀m≥m0n, ∀p∈N.
Consequently, the series∞k1xkyk converges inZ, and thereforex ≡ {xk}k∈N ∈ Ky. From
3.7it follows directly thatxn−xKy → 0, n → ∞. Thus,Kyis a Banach space. Let us consider the operatorK: Ky → Z, defined by the expression
Kx∞
n1
xnyn, x≡ {xn}n∈N. 3.11
It is obvious thatKis a linear operator. LetzKx. We have
K xZzZ∞
n1
xn yn
Z
≤ sup
m
m
n1
xn yn
Z
xKy. 3.12
It follows that K ∈ LKy;Z and K ≤ 1. Let x0 ≡ {x; 0;· · · }, x ∈ X. It is clear that Kx0Zx0Ky. Consequently,K1. It is absolutely obvious that if the system{yn}n∈N⊂
Y isb-linearly independent, then KerK {0}. In this case,∃K−1 : Z → Ky. If ImKis closed,
then, by the Banach’s theorem on the inverse operator, we obtain thatK−1 ∈ LImK;Ky.
The same considerations are valid in the case when the system{yn}n∈Nhas ab-biorthogonal
system. We will call operatorKa coefficient operator. Thus, we have proved the following.
Theorem 3.1. Every nondegenerate systemSy ≡ {yn}n∈N ⊂ Y is corresponded by a Banach space
of coefficientsKy and coefficient operatorK ∈ LKy;Z,K 1. If the system Sy isb-linearly
independent or has a b-biorthogonal system, then ∃K−1. Moreover, if ImK is closed, thenK−1 ∈
LImK;Ky.
In what follows, we will need the concept of b-basis in the space of coefficientsKy.
Definition 3.2. System {Tn}n∈N ⊂ LX; Ky is called b-basis in Ky if for for allx ∈
Ky,∃!{xn}n∈N⊂X:x ∞n1Tnxnconvergence inKy.
Consider the operatorsEn : X−→ Ky:Enx{δnkx}k∈N, n∈N. We have
EnxKy xynZ≤ynYxX, ∀x∈X. 3.13
Thus,En ∈LX;Ky, for alln∈N. Takex≡ {xn}n∈N∈ Ky. Then
x−
m
n1
Enxn
Ky
⎧ ⎨
⎩0; · · ·; 0;
m
xm 1;xm 2;· · ·
⎫ ⎬ ⎭
Ky
sup
p
mp
nm 1
xnyn
z
−→0, 3.14
as m → ∞, since the series ∞n1xnyn converges in Z. As a result, we obtain that x
∞
n1Enxn. Consider the operatorsPn :Ky → X:Pn xxn, n∈N. We have
PnxX xnX≤cnxnynZ≤cnsup
m
m
k1
xkyk
Z
Consequently,Pn∈LKy;X,n∈N. Let us show that the expansionx∞n1Enxnis unique.
Let∞n1Enxn 0. We have 0 Pk∞n1Enxn ∞n1PkEnxn xk,for allk ∈ N. As a result, we obtain that the system{En}n∈Nforms ab-basis forKy. We will call this system a
canonical system. So we have proved the following.
Theorem 3.3. Let Ky be a space of coefficients of nondegenerate system {yn}n∈N ⊂ Y. Then the
canonical system{En}n∈Nforms ab-basis forKy.
Let the nondegenerate system{yn}n∈N⊂Yform ab-basis forZ. Consider the coefficient
operatorK: Ky → Z. By definition of b-basis, the equationK xzis solvable with regard tox ∈ Ky for for allz ∈ Z. It is absolutely clear thatKerK {0}. Then it follows from Theorem 3.1and Banach theorem thatK−1 ∈LZ;Ky. Consequently, operatorK performs
isomorphism betweenKy and Z.
Vice versa, let{yn}n∈N⊂Y be a nondegenerate system and letKybe a corresponding
space of coefficients. Assume that a coefficient operatorK ∈ LKy;Zis an isomorphism.
Take for allz ∈Z. It is clear that∃x≡ {xn}n∈N∈ Ky : Kxz, that isz ∞n1xnyn inZ.
Consequently,zcan be expanded in a series with respect to the system{yn}n∈N. Let us show that such an expansion is unique. Let∞n1x0
nyn0 for somex0 ≡ {x0n}n∈N∈ Ky. This means
thatKx0 0⇒ x0 0⇒ xn0 0, for for alln∈N. Thus, the system{yn}n∈N forms a b-basis
for Z. So the following theorem is proved.
Theorem 3.4. LetKy be a space of coefficients of nondegenerate system{yn}n∈N and letK be a
corresponding coefficient operator. Then this system forms a b-basis for Z if and only if K is an
isomorphism inLKy; Z.
3.2. Criterion of Basicity
Let the systems{yn}n∈N⊂Y and{yn∗}n∈N ⊂LZ; Xbe b-biorthogonal. Take for allz∈Zand
consider the partial sums
Snz n
k1
y∗
kzyk, n∈N. 3.16
We have
SnSmz n
k1
y∗
kSmzyk n
k1
y∗
k
m
i1
y∗
izyi
yk
n
k1
m
i1
δkiyi∗zyk
min{n;m}
k1
y∗
kzykSmin{n;m}z, ∀n, m∈N.
3.17
Hence,S2
n Sn, for for alln ∈N, that is,Snis a projector inZ. It follows directly from the
estimate
y∗
thatSnis a continuous projector. Suppose that the nondegenerate system{yn}n∈N⊂Y forms
ab-basis forZ. Then for for allz∈Zhas a unique expansionz∞n1xnyninZ. We denote
the correspondencez → xnbyyn∗ :y∗nz xn, for alln∈N. It is obvious thaty∗n:Z → Xis
a linear operator. LetKybe a space of coefficients of basis{yn}n∈N, and letK:Ky → Zbe the
corresponding coefficient operator. ByTheorem 3.4,Kis an isomorphism. We have
y∗
nzX xnX≤cnxnyn≤cnsup m
m
k1
xkyk
Z
cnxKy
cnK−1z
Ky ≤cn
K−1zZ,
3.19
wherex≡ {xn}n∈N. Consequently,{yn∗}n∈N⊂LZ;X. It follows directly from the uniqueness
of the expansion thaty∗nxyk δnkx; for alln, k∈N, for for allx∈X. As a result, we obtain that the system{y∗n}n∈Nisb-biorthogonal to{yn}n∈N. Let us consider the projectorsSm∈LZ
for for allz∈Z:
Smz m
n1
y∗
nzyn, m∈N. 3.20
As the series3.20converges for for allz∈Z, it follows from Banach-Steinhaus theorem that
Msup
m Sm< ∞. 3.21
It is absolutely obvious that the system{yn}n∈Nis b-complete inZ. Thus, if the system{yn}n∈N
forms ab-basis forZ, then1it isb-complete inZ;2it has ab-biorthogonal system;3the corresponding family of projectors is uniformly bounded.
Vice versa, let the system{yn}n∈Nbeb-complete inZand have ab-biorthogonal system
{y∗
n}n∈N. Assume that the corresponding family of projectors{Sm}m∈Nis uniformly bounded,
that is, relation3.21holds. Letz∈Zbe an arbitrary element. Let us take arbitrary positive ε. It is clear that∃{xn}mn10 ⊂X: z−mn10 xnynZ< ε. Letz0mn10 xnyn. We have
y∗
nz0
m0
k1
y∗
nxkykxn, n1, m0;y∗nz0 0,∀n > m0. 3.22
As a result, we obtain form≥m0that
z−SmzZ≤ z−z0Z z0−SmzZ≤ε
m
n1
y∗
nz−z0yn
Z
≤M 1ε. 3.23
From the arbitrariness of ε we get limm→ ∞Smz z. Consequently, for for all z ∈ Z can
be expanded in a series with respect to the system {yn}n∈N. The existence ofb-biorthogonal
Theorem 3.5. Nondegenerate system{yn}n∈N⊂Y forms ab-basis forZif and only if the following
conditions are satisfied:
1the system isb-complete inZ;
2it has ab-biorthogonal system{y∗n}n∈N⊂LZ;X;
3the family of projectors3.21is uniformly bounded.
References
1 M. M. Day, Normed Linear Spaces, Izdat. Inostr. Lit., Moscow, Russia, 1961.
2 I. Singer, Bases in Banach Spaces, vol. 1, Springer, New York, NY, USA, 1970.
3 I. Singer, Bases in Banach Spaces, vol. 2, Springer, New York, NY, USA, 1981.
4 R. M. Young, An Introduction to Nonharmonic Fourier Series, Academic Press, New York, NY, USA, 1980.
5 B. T. Bilalov and S. G. Veliyev, Some problems of Basis, Elm, Baku, Azerbaijan, 2010.
6 Ch. Heil, A Basis Theory Primer, Springer, New York, NY, USA, 2011.
7 B. T. Bilalov and A. I. Ismailov, “Bases and tensor product,” Transactions of National Academy of Sciences
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