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Vol. 5, No. 1, 2012, 75-87

ISSN 1307-5543 – www.ejpam.com

SPECIALISSUE FOR THEINTERNATIONAL CONFERENCE ONAPPLIEDANALYSIS ANDALGEBRA 29 JUNE- 02 JULY2011, ISTANBULTURKEY

Statistical Approximation Properties of a Generalization of

Positive Linear Operators

Reyhan Canatan

1

, Ogün Do˘

gru

2,∗

1Department of Mathematics, Graduate School of Natural and Applied Science, Ankara University,

Gölba¸si, Ankara, Turkey

2Gazi University, Faculty of Science and Arts, Department of Mathematics, Teknik Okullar 06500,

Ankara, Turkey

Abstract. In the present paper, we introduce a generalization of positive linear operators and obtain its Korovkin type statistical approximation properties. The rates of statistical convergence of this gen-eralization is also obtained by means of modulus of continuity and Lipschitz type maximal functions. Secondly, we construct a bivariate generalization of these operators and investigate the statistical ap-proximation properties. We also get a partial differential equation such that the second moment of our bivariate operators is a particular solution of it. Finally, we obtain a Voronovskaja type formulae via statistical limit.

2000 Mathematics Subject Classifications: 41A10, 41A25, 41A36

Key Words and Phrases: Sequence of positive linear operators, Korovkin theorem for statistical ap-proximation, modulus of continuity, Lipschitz type maximal functions

1. Introduction

There are a lot of approximating operators that their Korovkin type error estimates, ap-proximation properties and rates of convergence are investigated (see[1]for details).

In the present paper, Korovkin type statistical approximation properties of a generalization of positive linear operators including many well-known operators which was defined by Do˘gru in[4]are investigated.

These operators are introduced as

Ln(f;x) = 1

ϕn(x)

X

ν=0

f( ν

an,ν)ϕ (ν)

n (0)

ν! (1)

Corresponding author.

Email addresses:reyhan.anatangmail.om(R. Canatan),ogun.dogrugazi.edu.tr(O. Do˘gru)

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R. Canatan, O. Do˘gru Eur. J. Pure Appl. Math,5(2012), 75-87 76

wherean,ν = ϕ (ν) n (0) ϕn−1)(0)

, lim ν→∞

an,ν

ν =µ, 0≤x <

1

µ and fC[0,

1

µ). Hereϕn(x)C∞satisfies the following conditions:

(i) Every element of the sequence ϕn is analytic on a domain D containing the disk B=nz∈C:|z|< 1µ

o

, (ii) ϕ(nν)(0) =

d xνϕn(x)|x=0>0 forν=1, 2, . . . ,

(iii) ϕn(x)>0 for eachx ∈[0,µ1),

(iv) There exists a sequence ofcn such that

aνn+,ν+11aνn,νcn

andst lim

n→∞cn=0.

Firstly, let us recall some notations and definitions on the concept of statistical conver-gence.

A sequence x = xk is said to be statistically convergent to a number of L if for every

ǫ >0,

δ¦k∈N:xkL

¾ǫ©=0 where δ(K):= lim

n 1

n{the numberkn:kK}whenever the limit exist[see e.g. 8]. For

instance,

δ(N) =1,δ{2k:k∈N}= 1

2 andδ

¦

k2:k∈N©=0.

Notice that any convergent sequence is statistically convergent but not conversely. For exam-ple, the sequence

xk=   

L1, n=m2, L2, n6=m2

(m=1, 2, 3, ...)

is statistically convergent to L2but not convergent in ordinary sense when L16=L2.

In this paper, we also define the bivariate operators for these operators and examine their statistical convergence and finally an application to partial differential equations is given.

2. Korovkin Type Statistical Approximation Properties

In [5], Gadjiev and Orhan proved the following Korovkin-type statistical approximation theorem for any sequence of positive linear operators.

(3)

satisfies the conditions

st−lim

n

An()−

C[a,b]=0,with eν(t) =t

ν,forν=0,1,2,

then, for any function fCM[a,b], we have

stlim

n

An(f)fC[a,b]=0.

The space of all functions f which are continuous in [a,b] and bounded all positive axis is denoted by CM[a,b].

To obtain main results of this part, let us recall some lemmas given in[4]

Lemma 1([4]). For all nN , x∈[0,a],(0<a< 1µ), we have

Ln(e0,x) =1. (2)

Lemma 2([4]). For all nN , x∈[0,a],(0<a< 1

µ), we have

Ln(e1,x) =x. (3) Lemma 3([4]). For all nN , x∈[0,a],(0<a< 1µ), we have

Ln(e2,x)−x2≤cnx. (4) Now, we can obtain the following main result for the operators given by (1).

Theorem 2. For all fCM[0,a],(0<a< µ1), we have

st−lim

n

Ln(f; .)−fC[0,a]=0.

Proof. By Lemma 1 and Lemma 2 it is clear that, st−lim

n

Ln(e0; .)−e0C[0,a]=0 (5)

and

st−lim

n

Ln(e1; .)−e1

C[0,a]=0. (6)

From Lemma 3, we have

Ln(e2; .)−e2

C[0,a]≤cna. (7)

Now, for a givenǫ >0, let us define the following sets:

T :=nk:Lk(e2; .)−e2C[0,a]¾ǫo

and

(4)

R. Canatan, O. Do˘gru Eur. J. Pure Appl. Math,5(2012), 75-87 78

We can see thatTT1by (7) so, we get

δnkn:Lk(e2; .)−e2

C[0,a]¾ǫ

o

δkn:cka¾ǫ .

Using thest− lim

n→∞cn=0 we have, st−lim

n

Ln(e2; .)−e2C[0,a]=0. (8)

Consequently, we can write st−lim

n

Ln(eν; .)−eνC[0,a]=0, forν=0, 1, 2. (9)

So the proof is completed from Theorem 1.

3. Rates of Statistical Convergence

Let fC[0,a], the modulus of continuity of f, denoted byω(f,δ)is defined as

ω(f,δ):= sup

x,t∈[0,a],|tx|≤δ

f(t)−f(x). (10)

At this point let us recall following theorems which were proved in[4]. Theorem 3([4]). Let fC[0,a]. If Ln is defined by(1), then we have

Ln(f; .)− f

(1+pa)ω(f,pcn) (11)

whereω(f,pcn)is modulus of continuity defined in(10)andnlim→∞cn=0.

The Lipschitz type maximal functions of orderαintroduced by Lenze[7]as follows

e

ωα(f,x):= sup

t6=x;t∈[0,a]

f(t) f(x)

|tx|α , x∈[0,a], α∈(0, 1]. Notice that, the boundedness ofωeα(f,x)is equivalent to fLipM(α).

Now let us compute the rate of convergence for the differenceLn(f;x)−f(x)with the help of Lipschitz type maximal functions.

Theorem 4([4]). If Lnis defined by(1), then we have

Ln(f;x) f(x) cnx

α

2ωe

α(f,x). (12)

Remark 1. Achieving a fast order of statistical convergence is important in approximation by positive linear operators. If we replace lim

n→∞cn=0by stnlim→∞cn=0in Theorem 3 and Theorem 4, it is obvious that

st− lim

n→∞ω(f,

pc

n) =0.

(5)

4. Construction of the Bivariate Operators

Let I2= [0,a]×[0,a],(0<a<µ1), and fC([0,a]2)

Lnx f;x,y= 1

ϕn(x)

X

ν=0

f

‚

ν

an,ν ,y

Œ

ϕ(nν)(0)x

ν

ν! and

Lmy f;x,y= 1

ϕm y

X

η=0

f

‚

x, η bm,η

Œ

ϕ(mη)(0)y

η

η! where

an,ν =

ϕ(nν)(0)

ϕ(nν−1)(0), limν→∞

an,ν

ν =µ, 0≤ x<

1

µ and fC([0,

1

µ)×[0,

1

µ))

and

bm,η= ϕ

(η)

m (0)

ϕ(mη−1)(0)

, lim η→∞

bm,η

η =µ, 0≤ y <

1

µ and fC([0,

1

µ)×[0,

1

µ)).

Hereϕn(x)C∞andϕm yC∞satisfy the following conditions:

(a) Every element of the sequenceϕn andϕm are analytic on a domain Dcontaining the diskB=nz∈C:|z|< µ1o,

(b) ϕ(nν)(0) =

d xνϕn(x)|x=0 > 0 for ν = 1, 2, . . . , and ϕ

(η)

m (0) = d η

d yηϕm(y)

y=0 > 0 for

η=1, 2, . . . ,

(c) ϕn(x)>0 for eachx ∈[0,µ1), andϕm y>0 for each y ∈[0,µ1),

(d) There exists a sequence ofcn such that

aν+1

n,ν+1 −

ν

an,ν

cn andst− lim

n→∞cn =0 and a

sequence ofdm such that bη+1

m,η+1−

η

bm,η

dmandstmlim→∞dm=0.

Now we can define the following bivariate generalization of linear and positive operators

Ln,m f;x,y

= 1

ϕn(x)

1

ϕm y

X

ν=0

X

η=0

f

‚

ν

an,ν,

η

bm,η

Œ

ϕ(nν)(0)ϕ(mη)(0)x

ν

ν!

η!. (13) Lemma 4. For the operators(13), we have

Ln,m f;x,y=Lnx€Lmy f;x,yŠ=Lmy €Lnx f;x,yŠ. Proof. Following calculations reveal that

Lnx€Lmy f;x,yŠ = 1

ϕm y

X

η=0

1

ϕn(x)

X

ν=0

f

‚

ν

an,ν , η

bm,η

Œ

ϕn(ν)(0)x

ν

ν!ϕ (η)

m (0)

(6)

R. Canatan, O. Do˘gru Eur. J. Pure Appl. Math,5(2012), 75-87 80

= 1

ϕn(x)

1

ϕm y

X

ν=0

X

η=0

f

‚

ν

an,ν , η

bm,η

Œ

ϕn(ν)(0)ϕ(mη)(0)x

ν

ν!

η!

= Ln,m f;x,y. Similarly we can easily show that Lmy

€

Lnx f;x,yŠ=Ln,m f;x,y

.

5. Statistical Approximation Properties of the Bivariate Operators

If we have

st−lim

n,m

fn,mf

C([a,b]×[c,d])=0 then we say that the sequence of functions ¦fn,m

©

statistically convergent to f uniformly.

Where

f

C([a,b]×[c,d])= max

(x,y)∈[a,b]×[c,d]

f x,y.

Volkov[9]gave the first Korovkin type theorem for bivariate functions. Subsequently, H.H. Gonska, C. Badea and I. Badea established a simpler form of Volkov’s theorem as follows: Theorem 5([6]). Let a, b, c, d be real numbers satisfying the inequalities a< b, c<d and let

Ln,m:C([a,b]×[c,d])→C([a,b]×[c,d])

be a positive linear operators having the properties for any x,y∈[a,b]×[c,d]

(1) Ln,m e00;x,y=1+un,m x,y, (2) Ln,m e10;x,y=x+vn,m x,y, (3) Ln,m e01;x,y

= y+wn,m x,y

,

(4) Ln,m e20+e02;x,y=x2+y2+hn,m x,y. If the sequences ¦un,m x,y

©

, ¦vn,m x,y ©

, ¦wn,m x,y ©

, ¦hn,m x,y ©

converge to zero uniformly on [a,b]×[c,d], then (Ln,mf) converges to f uniformly on[a,b]×[c,d]for any

fC([a,b]×[c,d])where ei,j=xiyj are two dimensional test functions.

Lemma 5. The bivariate operators in(13)satisfy the following items: (i) Ln,m e00;x,y=1,

(ii) Ln,m e10;x,y

=x ,

(iii) Ln,m e01;x,y= y,

(iv) Ln,m e20+e02;x,yx2−ycnx+dmy where cn and dn satisfy the properties in

(7)

Proof.

(i) It is obvious that

Ln,m e00;x,y

= Ln,m 1;x,y

= 1

ϕn(x)

1

ϕm y

X

ν=0

X

η=0

ϕ(nν)(0)ϕm(η)(0)x

ν

ν!

η!. By using Lemma 1, we have Ln,m e00;x,y=1.

(ii)

Ln,m e10;x,y= 1

ϕn(x)

1

ϕm y

X

ν=0

X

η=0

ν

an,ν

ϕ(nν)(0)ϕ(mη)(0)x

ν

ν!

η! by using Lemma 2, we can easily see thatLn,m e10;x,y

= x. (iii) It is proven by similarly way like(ii).

(iv) Since

Ln,m e20+e02;x,y = 1

ϕn(x)

1

ϕm y

X

ν=0

X

η=0   ‚

ν

an,ν

Œ2 +

‚

η

bm,η

Œ2 

×ϕ(nν)(0)ϕm(η)(0)x

ν

ν!

η!, by using Lemma 3 the proof is completed.

Theorem 6. The sequence€Ln,mfŠdefined by(13)converges statistically to fC([0,a]×[0,a])

uniformly in[0,a]×[0,a]. Proof.

st−lim

n,m

Ln,m e00; ., .

e00

=0, (14)

st−lim

n,m

Ln,m e10; ., .−e10=0, (15) st−lim

n,m

Ln,m e01; ., .−e01=0 (16)

and from the property(d), we can easily obtain st−lim

n,m

Ln,m e20+e02; ., .

e20−e02

=0. (17)

Using (14), (15), (16), (17), in the light of Theorem 3, we have st−lim

n,m

(8)

R. Canatan, O. Do˘gru Eur. J. Pure Appl. Math,5(2012), 75-87 82

6. Estimation of the Rate of Statistical Convergence of the Bivariate Operators

Definition 1([2]). I2= [0,a]×[0,a], fC€Ifor anyδ1>0,δ2>0

ω f;δ1,δ2= sup (t,s)∈I2,(x,y)∈I2

|tx|≤δ1,|sy|≤δ2

f (t,s)−f x,y. (19)

Theorem 7. If€Ln,mfŠis defined by(13)then we have

Ln,m f; ., .−fC(I2)ω

f;pcn,pdm €pa+1Š2. (20) Proof. Using the properties for modulus (19), we have

f (t,s)− f x,yω f;δ1,δ2

|tx|

δ1 +1

sy

δ2 +1

!

. (21)

On the other hand, for anyn∈N, x,yI2 we have

Ln,m f;x,y

f x,yLn,m€f (t,s) f x,y;x,yŠ. (22) If we use (21) in (22), then we get

Ln,m f;x,yf x,yω f;δ1,δ2

×Ln,m |tx|

δ1 +1

sy

δ2 +1

!

;x,y

!

= ω f;δ1,δ2 1 δ1δ2

1

ϕn(x)

1

ϕm y

× ∞

X

ν=0

X

η=0

ν

an,νx

η

bm,ηy

ϕ

(ν)

n (0)ϕ

(η)

m (0)

×x ν

ν!

η!

+ω f;δ1,δ2 1 δ1

1

ϕn(x)

1

ϕm y

× ∞

X

ν=0

X

η=0

ν

an,νx

ϕ()(0)ϕ

(η)

m (0)

ν!

η!

+ω f;δ1,δ2 1

δ2

1

ϕn(x)

1

ϕm y

X

ν=0

X

η=0

η

bm,ηy

×ϕ(nν)(0)ϕ(mη)(0)x

ν

ν!

η! +ω f;δ1,δ2

(9)

By using Cauchy-Schwarz inequality and Lemmas 1, 2 and 3, then we obtain

Ln,m f;x,yf x,yω f;δ1,δ2

δ1δ2

×

 1

ϕn(x)

X

ν=0 ‚

ν

an,νx

Œ2

ϕ(nν)(0)x

ν

ν!

 

1 2

×

 1

ϕm y

X

η=0 ‚

η

bm,ηy

Œ2

ϕ(mη)(0)y

η

η!

 

1 2

+ω f;δ1,δ2

δ1

×

 1

ϕn(x)

X

ν=0 ‚

ν

an,νx

Œ2

ϕ(nν)(0)x

ν

ν!

 

1 2

+ω f;δ1,δ2

δ2

×

 1

ϕm y

X

η=0 ‚

η

bm,ηy

Œ2

ϕ(mη)(0)y

η

η!

 

1 2

+ω f;δ1,δ2

= ω f;δ1,δ2

δ1δ2

cnx12 d

my 1

2 +ω f;δ1,δ2

δ1

cnx12

+ω f;δ1,δ2

δ2

dmy12+ω f;δ

1,δ2

.

If we chooseδ1=pcn,δ2= p

dm in the last inequality then we have

Ln,m f; ., .−fC(I2)ω

f;pcn,pdm

p

apa+ω

f;pcn,pdm

p

a

+ωf;pcn,pdmpa+ωf;pcn,pdm

= ω

f;pcn,pdm €a+2pa+1Š

= ω

f;pcn, p

dm €p

a+1Š2.

Remark 2. Since cnand dmsatisfy st− lim

n→∞cn=0and stmlim→∞dm=0, we can easily say that

€€

Ln,mfŠŠis statistically convergent to f on I2.

7. Application to Partial Differential Equations

Let€€Ln,mf ŠŠ

(10)

R. Canatan, O. Do˘gru Eur. J. Pure Appl. Math,5(2012), 75-87 84

Theorem 8. Let

d

d xϕn(x) =hn(x)ϕn(x), (23) d

d yϕm y

=hm m y (24)

and

g

‚

ν

an,ν , η

bm,η

Œ = ν

sn + η

tm

. (25)

Then we have

x sn

∂xLn,m f;x,y

+ y

tm

yLn,m f;x,y

=

x

snhn(x)− y tmhm y

×Ln,m f;x,y

+Ln,m f g;x,y

. (26) Proof. Using the equalities

∂xLn,m f;x,y

= −ϕ

n(x)

ϕ2n(x)

1

ϕm y

× ∞

X

ν=0

X

η=0

f

‚

ν

an,ν,

η

bm,η

Œ

ϕ(nν)(0)ϕ(mη)(0)x

ν

ν!

η!

+ 1

ϕn(x)ϕm y

× ∞

X

ν=0

X

η=0

f

‚

ν

an,ν,

η

bm,η

Œ

ϕn(ν)(0)ϕm(η)(0)νx

ν−1

ν!

η! and

∂yLn,m f;x,y

= −ϕ

m y

ϕ2m y 1

ϕn(x)

× ∞

X

ν=0

X

η=0

f

‚

ν

an,ν , η

bm,η

Œ

ϕ(nν)(0)ϕ(mη)(0)x

ν

ν!

η!

+ 1

ϕn(x)ϕm y

× ∞

X

ν=0

X

η=0

f

‚

ν

an,ν,

η

bm,η

Œ

ϕ(nν)(0)ϕ(mη)(0)x

ν

ν!

ηyη−1

(11)

8. Voronovskaja Type Approximation Properties

It can be given the following theorem for Voronovskaja type operators via statistical limit. Lemma 6. It can be easily showed that

Ln €

t3;xж x3+3x2cn+x c2n (27)

and

Ln €

t4;xжx4+6cnx3+4cn2x 2+c3

nx (28)

Theorem 9. Let Ln f;x

as in(1)

st− lim

n−→∞ 1 cn

Ln(t;x)−f (x)= f

′′

(x)

2 x (29)

Proof. Proof. Necessity. It will be used the same technique in[3]for this proof. It is known from the Taylor expansion

f(t) = f(x) +f′(x) (tx) + f

′′

(x)

2 (tx)

2η(

tx) (30)

where η(tx) = f

′′′

(x)

3! (tx) +. . . and it is a continuous function and tends to zero for

tx.

Let’s chooset = aν

n,ν in(30)then

f

‚

ν

an,ν

Œ

= f(x) +f′(x) ‚

ν

an,νx

Œ + f

′′

(x)

2

‚

ν

an,νx

Œ2 +

‚

ν

an,νx

Œ2

η( ν

an,νx). (31) Sinceηis a continuous function, it is bounded and there exists a positive constantH, so for allh, we can writeη(hH. If (31) is multiplied with 1

ϕn(x)ϕ

(ν)

n (0)

ν! and taken sum

fromν =0 to infinity from both side of it, we have 1

ϕn(x)

X

ν=0

f( ν

an,ν)ϕ (ν)

n (0)

ν! = f(x)Ln(1;x) +f(x)L

n(tx;x)

+f

′′

(x)

2 Ln

€

(tx)2;xŠ

+ 1

ϕn(x)

X

ν=0 ( ν

an,νx)

2η ‚

ν

an,νx

Œ

ϕn(ν)(0)x

ν

ν! so

Ln f;x= f (x) +f′(x)Ln(t;x)−x+ f

′′

(x)

2

”

(12)

R. Canatan, O. Do˘gru Eur. J. Pure Appl. Math,5(2012), 75-87 86

where

I= 1

ϕn(x)

X

ν=0 ( ν

an,νx)2η

‚

ν

an,νx

Œ

ϕn(ν)(0)x

ν

ν!

= 1

ϕn(x)

X

ν=0 anν,νx

δ

( ν

an,νx)

2η ‚

ν

an,νx

Œ

ϕn(ν)(0)x

ν

ν!

+ 1

ϕn(x)

X

ν=0 anν,νx

( ν

an,νx)2η

‚

ν

an,νx

Œ

ϕ(nν)(0)x

ν

ν! (33)

Becauseηis a continuous function for everyǫ >0 there exists aδ(ǫ),

η  ν

an,νx ‹

ǫ

andηis bounded for

aν

n,νx

> δwe have

η  ν

an,νx ‹

<H. If these expressions are used

in (33), we have

Iǫ 1 ϕn(x)

X

ν=0 ( ν

an,ν

x)2ϕ(nν)(0)x

ν

ν! +H J (34)

where

J = 1

ϕn(x)

X

ν=0 anν,νx

( ν

an,ν

x)2ϕ(nν)(0)x

ν

ν! (35)

Due to

aν

n,νx > δ,

( ν

an,νx)

2

δ2 >1. So

J¶ 1

δ2

1

ϕn(x)

X

ν=0 ( ν

an,ν

x)4ϕ(nν)(0)x

ν

ν!. (36)

By using (34) and (36)

IǫLn€(tx)2;xŠ+H 1

δ2Ln €

(tx)4;xŠ (37) and using (28) in (37) we obtain

Ln(t;x)−f (xcn

 f

′′

(x)

2 x+ǫx+ H

δ2x c 2 n

 ,

so

Ln(t;x)−f(x) =o(cn)  f

′′

(x)

2 x+ǫx+ H

δ2x c 2 n

 

Becausest− lim

(13)

Remark 3. It is obvious that since cntends to zero statistically, we have a better order of approx-imation in Theorem 9 than Theorem 3.

References

[1] F. Altomore and M. Campiti.Korovkin Type Approximation Theory and its Applications. Walter de Gruyter, Berlin, 1994.

[2] G. Anastassiou and S. Gal. Approximation Theory: Moduli of Continuity and Global Smoothness Preservation. Birkhäuser, Boston, 2000.

[3] O. Do˘gru. Necessary conditions to obtain Voronovskaja type asymptotic formulae via statistical limit.Proc. of the 12th WSEAS Int. Conf. on Applied Mathematics.,pages 128-131, Cairo, Egypt, 2007.

[4] O. Do˘gru. Approximation properties of a generalization of positive linear operators.J. Math. Anal. Appl., 342:161-170, 2008.

[5] A. Gadjiev and C. Orhan. Some Approximation Theorems via statistical convergence. Rocky Mountain J. Math., 32:129-138, 2002.

[6] H. Gonska, C. Badea and I. Badea. A Test Function Theorem and Approximation by Pseudopolynomials.Bull. Austral. Math. Soc., 34:53-64, 1986.

[7] B. Lenze. Bernstein-Baskakov-Kantorovich Operators and Lipschitz-Type maximal func-tions.in: Approx. Th. Kecskemét, Hungary, Colloq. Math. Soc. János Bolyai,. 58:469-496, 1990.

[8] I. Niven, H. Zuckerman and H. Montgomery.An Introduction to the Theory of Numbers. 5th Edition, Wiley, New York, 1991.

References

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