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Chlodowsky variant of q-Bernstein-Schurer-Stancu operators

Abstract

It was Chlodowsky who considered non-trivial Bernstein operators, which help to approximate bounded continuous functions on the unbounded domain. In this paper, we introduce the Chlodowsky variant of q-Bernstein-Schurer-Stancu operators. By obtaining the first few moments of these operators, we prove Korovkin-type approximation theorems in different function spaces. Furthermore, we compute the error of the approximation by using the modulus of continuity and Lipschitz-type functionals. Then we obtain the degree of the approximation in terms of the modulus of continuity of the derivative of the function. Finally, we study the generalization of the Chlodowsky variant of q-Bernstein-Schurer-Stancu operators and investigate their approximations.

MSC:41A10, 41A25, 41A36.

1 Introduction

The classical Bernstein-Chlodowsky operators were defined by Chlodowsky [1] as

C n (f;x)= r = 0 n f ( r n b n ) ( n r ) ( x b n ) r ( 1 x b n ) n r ,

where the function f is defined on [0,) and ( b n ) is a positive increasing sequence with b n and b n n 0 as n.

In 1968, Stancu [2] constructed and studied the Bernstein-Stancu operators, which were defined as

P m α , β (f;x)= k = 0 m f ( k + α m + β ) ( m k ) x k ( 1 x ) m k ,

where α,βR such that 0αβ.

In 1987, Lupaş [3] introduced the q-based Bernstein operators and obtained the Korovkin-type approximation theorem. In 1996, other q-based Bernstein operators were defined by Phillips [4, 5]. During the last decade q-based operators have become an active research area (see [69]).

In 2011, the q-Bernstein-Schurer operators were defined by Muraru [10], for fixed p N 0 and for all x[0,1], by

B n p (f;q;x)= k = 0 n + p f ( [ k ] [ n ] ) [ n + p k ] x k s = 0 n + p k 1 ( 1 q s x ) ,
(1.1)

where q is a positive real number and the function f is evaluated at the q-integers [ k ] [ n ] . Recall that the q-integer of kR is [11]

[k]={ ( 1 q k ) / ( 1 q ) , q 1 , k , q = 1 ,

the q-factorial is defined by

[k]!={ [ k ] [ k 1 ] [ 1 ] , k = 1 , 2 , 3 , , 1 , k = 0

and q-binomial coefficients are defined by

[ n k ]= [ n ] ! [ n k ] ! [ k ] !

for n0, k0. Note that the case q 1 in (1.1), the operators defined by (1.1) were reduced to the operators considered by Schurer [12].

Some properties of the q-Bernstein-Schurer operators were investigated in [13]. We should notice that the case p=0 reduces to the q-Bernstein operators.

It should be noted that complex approximation properties of some Schurer-type operators were investigated in [14, 15] and [16].

Recently, Barbosu investigated Schurer-Stancu operators S m , p α , β :C[0,1+p]C[0,1] which were defined by [17] (see also [18])

S m , p α , β (f;x)= k = 0 m + p f ( k + α m + β ) ( m + p k ) x k ( 1 x ) m + p k ,
(1.2)

where α and β are non-negative numbers which satisfy 0αβ and also p is a non-negative integer.

In 2008, Karslı and Gupta [19] defined the q-analogue of Chlodowsky operators by

C n (f;q;x)= k = 0 n f ( [ k ] [ n ] b n ) [ n k ] ( x b n ) k s = 0 n k 1 ( 1 q s x b n ) ,0x b n ,

where ( b n ) has the same property of Bernstein-Chlodowsky operators.

Lately, the q-analogues of Bernstein-Schurer-Stancu operators were introduced by Agrawal et al. as [20]

S n , p α , β (f;q;x)= k = 0 n + p f ( [ k ] + α [ n ] + β ) [ n + p k ] x k s = 0 n + p k 1 ( 1 q s x ) ,

where α, β and p are non-negative integers such that 0αβ. For the first few moments, we have the following lemma.

Lemma 1.1 [[20], p.7755]

For the operator S n , p α , β (f;q;x), we have the following moments:

(i) S n , p α , β ( 1 ; q ; x ) = 1 , (ii) S n , p α , β ( t ; q ; x ) = [ n + p ] x + α [ n ] + β , (iii) S n , p α , β ( t 2 ; q ; x ) = 1 ( [ n ] + β ) 2 ( [ n + p ] 2 x 2 + [ n + p ] x ( 1 x ) + 2 α [ n + p ] x + α 2 ) .

The organization of the paper as follows.

In Section 2, we introduce the Chlodowsky variant of q-Bernstein-Schurer-Stancu operators and investigate the moments of the operator. In Section 3, we study several Korovkin-type theorems in different function spaces. In Section 4, we obtain the order of convergence of the Chlodowsky variant of q-Bernstein-Schurer-Stancu operators by means of Lipschitz class functions and the first modulus of continuity. In addition, we calculate the degree of convergence of the approximation process in terms of the first modulus of continuity of the derivative of the function. In Section 5, we study the generalization of the Chlodowsky variant of q-Bernstein-Schurer-Stancu operators and investigate their approximations.

2 Construction of the operators

We construct the Chlodowsky variant of q-Bernstein-Schurer-Stancu operators as

C n , p ( α , β ) (f;q;x):= k = 0 n + p f ( [ k ] + α [ n ] + β b n ) [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) ,
(2.1)

where nN and p N 0 and α,βR with 0αβ, 0x b n , 0<q<1. Clearly, C n , p ( α , β ) is a linear and positive operator. Note that the cases q1 and p=0 in (2.1) reduce to the Stancu-Chlodowsky polynomials [21].

Firstly, we obtain the following lemma, which will be used throughout the paper.

Lemma 2.1 Let C n , p ( α , β ) (f;q;x) be given in (2.1). Then the first few moments of the operators are

(i) C n , p ( α , β ) ( 1 ; q ; x ) = 1 , (ii) C n , p ( α , β ) ( t ; q ; x ) = [ n + p ] x + α b n [ n ] + β , (iii) C n , p ( α , β ) ( t 2 ; q ; x ) = 1 ( [ n ] + β ) 2 { [ n + p 1 ] [ n + p ] q x 2 + ( 2 α + 1 ) [ n + p ] b n x + α 2 b n 2 } , (iv) C n , p ( α , β ) ( ( t x ) ; q ; x ) = ( [ n + p ] [ n ] + β 1 ) x + α b n [ n ] + β , (v) C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) = ( [ n + p 1 ] [ n + p ] q ( [ n ] + β ) 2 2 [ n + p ] [ n ] + β + 1 ) x 2 C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) = + ( ( 2 α + 1 ) [ n + p ] ( [ n ] + β ) 2 2 α [ n ] + β ) b n x + α 2 b n 2 ( [ n ] + β ) 2 .

Proof Using Lemma 1.1 and considering the following facts:

C n , p α , β ( 1 ; q ; x ) = S n , p α , β ( 1 ; q ; x b n ) , C n , p α , β ( t ; q ; x ) = b n S n , p α , β ( t ; q ; x b n ) , C n , p α , β ( t 2 ; q ; x ) = b n 2 S n , p α , β ( t 2 ; q ; x b n ) ,

we get the assertions (i), (ii), and (iii).

Using the linearity of the operators, we have

C n , p ( α , β ) ( ( t x ) ; q ; x ) = C n , p ( α , β ) ( t ; q ; x ) x C n , p ( α , β ) ( 1 ; q ; x ) = ( [ n + p ] [ n ] + β 1 ) x + α b n [ n ] + β .

So, we get (iv).

Similar computations give

C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) = C n , p ( α , β ) ( t 2 ; q ; x ) 2x C n , p ( α , β ) (t;q;x)+ x 2 C n , p ( α , β ) (1;q;x).

Then we have

C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) = ( [ n + p 1 ] [ n + p ] ( [ n ] + β ) 2 q 2 [ n + p ] [ n ] + β + 1 ) x 2 + ( ( 2 α + 1 ) [ n + p ] ( [ n ] + β ) 2 2 α [ n ] + β ) b n x + α 2 b n 2 ( [ n ] + β ) 2 .

This proves (v). □

Lemma 2.2 For each fixed q(0,1), we have

[ n + p 1 ] [ n + p ] ( [ n ] + β ) 2 q2 [ n + p ] [ n ] + β +1 ( q n [ p ] β ) 2 ( [ n ] + β ) 2 .

Proof Since [n+p1][n+p]q [ n + p ] 2 we get

[ n + p 1 ] [ n + p ] ( [ n ] + β ) 2 q2 [ n + p ] [ n ] + β +1 ( [ n + p ] [ n ] + β 1 ) 2 .

If we calculate the right-hand side of the above inequality, we get the following:

[ n + p 1 ] [ n + p ] ( [ n ] + β ) 2 q 2 [ n + p ] [ n ] + β + 1 1 ( [ n ] + β ) 2 { ( 1 q n + p ) 2 ( 1 q ) 2 2 ( 1 q n + p ) ( 1 q n ) ( 1 q ) 2 2 β ( 1 q n + p ) 1 q + ( 1 q n ) 2 ( 1 q ) 2 + 2 β ( 1 q n ) 1 q + β 2 } = 1 ( [ n ] + β ) 2 { q 2 n ( q 2 p 2 q p + 1 ) ( 1 q ) 2 + 2 β q n ( q p 1 ) 1 q + β 2 } = 1 ( [ n ] + β ) 2 { q 2 n ( 1 q p ) 2 ( 1 q ) 2 2 β q n ( 1 q p ) 1 q + β 2 } = 1 ( [ n ] + β ) 2 { q 2 n [ p ] 2 2 β q n [ p ] + β 2 } = ( q n [ p ] β ) 2 ( [ n ] + β ) 2 .

 □

Remark 2.1 As a consequence of Lemma 2.1 and Lemma 2.2, we have

C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) ( q n [ p ] β ) 2 ( [ n ] + β ) 2 x 2 + ( ( 2 α + 1 ) [ n + p ] ( [ n ] + β ) 2 ) b n x+ α 2 b n 2 ( [ n ] + β ) 2 .
(2.2)

Lemma 2.3 For the second central moment we have the following estimate:

sup 0 x b n C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) ( q n [ p ] β ) 2 ( [ n ] + β ) 2 b n 2 + ( ( 2 α + 1 ) [ n + p ] ( [ n ] + β ) 2 ) b n 2 + α 2 b n 2 ( [ n ] + β ) 2 .

Proof Taking supremum over [0, b n ] in (2.2) we get the result. □

3 Korovkin-type approximation theorem

In this section, we prove Korovkin-type approximation theorem for the Chlodowsky variant of q-Bernstein-Schurer-Stancu operators. Denote by C ρ the space of all continuous functions f, satisfying the condition

|f(x)| M f ρ(x),<x<.

Obviously, C ρ is a linear normed space with the norm

f ρ = sup < x < | f ( x ) | ρ ( x ) .

In studying the weighted approximation, the following theorem is crucial.

Theorem 3.1 (See [22])

There exists a sequence of positive linear operators T n , acting from C ρ to C ρ , satisfying the conditions

lim n T n ( 1 ; x ) 1 ρ =0,
(3.1)
lim n T n ( ϕ ; x ) ϕ ρ =0,
(3.2)
lim n T n ( ϕ 2 ; x ) ϕ 2 ρ =0,
(3.3)

where ϕ(x) is continuous and increasing function on (,) such that lim x ± ϕ(x)=± and ρ(x)=1+ ϕ 2 and there exists a function f C ρ for which lim n ¯ T n f f ρ >0.

The following theorem has been given in [22] and will be used in the investigation of the approximation properties of C n , p ( α , β ) (f;q;x) in weighted spaces.

Theorem 3.2 (See [22])

The conditions (3.1), (3.2), (3.3) imply lim n T n f f ρ =0 for any function f belonging to the subset C ρ 0 of C ρ for which

lim | x | f ( x ) ρ ( x )

exists finitely.

Particularly, choosing ρ(x)=1+ x 2 and applying Theorem 3.2 to the operators

T n α , β (f;q;x)={ C n , p ( α , β ) ( f ; q ; x ) if  0 x b n , f ( x ) if  x [ 0 , b n ] ,

we can state the following theorem.

Theorem 3.3 For all f C 1 + x 2 0 we have

lim n sup 0 x b n | T n α , β ( f ; q n ; x ) f ( x ) | 1 + x 2 =0

provided that q:=( q n ) with 0< q n <1, lim n q n =1 and lim n b n [ n ] =0 as n.

Proof In the proof we directly use Theorem 3.2. Obviously, by Lemma 2.1(i), (ii), and (iii) we get the following inequalities, respectively:

sup 0 x b n | T n α , β ( t ; q n ; x ) x | 1 + x 2 sup 0 x b n | ( [ n + p ] [ n ] + β 1 ) | x + α b n [ n ] + β ( 1 + x 2 ) | [ n + p ] [ n ] + β 1 | + α b n [ n ] + β 0

and

sup 0 x b n | T n α , β ( t 2 ; q n ; x ) x 2 | 1 + x 2 sup 0 x b n | [ n + p 1 ] [ n + p ] q n ( [ n ] + β ) 2 | x 2 + ( 2 α + 1 ) [ n + p ] b n x + α 2 b n 2 ( [ n ] + β ) 2 ( 1 + x 2 ) | [ n + p 1 ] [ n + p ] q n ( [ n ] + β ) 2 | + ( 2 α + 1 ) [ n + p ] b n + α 2 b n 2 ( [ n ] + β ) 2 0

is satisfied since lim n q n =1 and b n [ n ] 0 as n. □

Lemma 3.4 Let A be a positive real number independent of n and f be a continuous function which vanishes on [A,]. Assume that q:=( q n ) with 0< q n <1, lim n q n n =K< and lim n b n 2 [ n ] =0. Then we have

lim n sup 0 x b n | C n , p ( α , β ) (f; q n ;x)f(x)|=0.

Proof From the hypothesis on f, one can write |f(x)|M (M>0). For arbitrary small ε>0, we have

|f ( [ k ] + α [ n ] + β b n ) f(x)|<ε+ 2 M δ 2 ( [ k ] + α [ n ] + β b n x ) 2 ,

where x[0, b n ] and δ=δ(ε) are independent of n. With the help of the following equality:

k = 0 n + p ( [ k ] + α [ n ] + β b n x ) 2 [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) = C n , p ( α , β ) ( ( t x ) 2 ; q n ; x ) ,

we get by Theorem 3.3 and Remark 2.1

sup 0 x b n | C n , p ( α , β ) ( f ; q n ; x ) f ( x ) | ε + 2 M δ 2 [ ( q n n [ p ] β ) 2 ( [ n ] + β ) 2 b n 2 + ( ( 2 α + 1 ) [ n + p ] ( [ n ] + β ) 2 ) b n 2 + α 2 b n 2 ( [ n ] + β ) 2 ] .

Since b n 2 [ n ] 0 as n, we have the desired result. □

Theorem 3.5 Let f be a continuous function on the semi-axis [0,) and

lim x f(x)= k f <.

Assume that q:=( q n ) with 0< q n <1, lim n q n =1, lim n q n n =K<, and lim n b n 2 [ n ] =0. Then

lim x sup 0 x b n | C n , p ( α , β ) (f; q n ;x)f(x)|=0.

Proof The proof will be given along the lines of the proof of Theorem 2.5 in [23]. Clearly, it is sufficient to prove the theorem for the case k f =0. Since lim x f(x)=0, given any ε>0 we can find a point x 0 such that

|f(x)|ε,x x 0 .
(3.4)

For any fixed c>0, define an auxiliary function as follows:

g(x)={ f ( x ) , 0 x x 0 , f ( x 0 ) f ( x 0 ) c ( x x 0 ) , x 0 x x 0 + c , 0 , x x 0 + c .

Then for sufficiently large n in such a way that b n x 0 +c and in view of sup x 0 x x 0 + c |g(x)|=|f( x 0 )|, we have

sup 0 x b n | f ( x ) g ( x ) | sup x 0 x x 0 + c | f ( x ) g ( x ) | + sup b n x x 0 + c | f ( x ) | 2 sup x 0 x x 0 + c | f ( x ) | + sup b n x x 0 + c | f ( x ) | .

We have from (3.4)

sup 0 x b n |f(x)g(x)|3ε.

Now, we can write

sup 0 x b n | C n , p ( α , β ) ( f ; q n ; x ) f ( x ) | sup 0 x b n | C n , p ( α , β ) ( | f g | ; q n ; x ) | + sup 0 x b n | C n , p ( α , β ) ( g ; q n ; x ) g ( x ) | + sup 0 x b n | f ( x ) g ( x ) | 6 ε + sup 0 x b n | C n , p ( α , β ) ( g ; q n ; x ) g ( x ) | ,

where g(x)=0 for x 0 +cx b n . By Lemma 3.4, we obtain the result. □

4 Order of convergence

In this section, we compute the rate of convergence of the operators in terms of the elements of Lipschitz classes and the modulus of continuity of the function. Additionally, we calculate the order of convergence in terms of the first modulus of continuity of the derivative of the function.

Now, we give the rate of convergence of the operators C n , p ( α , β ) in terms of the Lipschitz class Lip M (γ), for 0<γ1. Let C B [0,) denote the space of bounded continuous functions on [0,). A function f C B [0,) belongs to Lip M (γ) if

|f(t)f(x)|M|tx | γ ( t , x [ 0 , ) )

is satisfied.

Theorem 4.1 Let f Lip M (γ)

| C n , p ( α , β ) ( f ; q ; x ) f ( x ) | M ( λ n ( x ) ) γ / 2 ,

where λ n , q (x)=( ( q n n [ p ] β ) 2 ( [ n ] + β ) 2 ) x 2 +( ( 2 α + 1 ) [ n + p ] ( [ n ] + β ) 2 2 α [ n ] + β ) b n x+ α 2 b n 2 ( [ n ] + β ) 2 .

Proof Considering the monotonicity and the linearity of the operators, and taking into account that f Lip M (γ),

| C n , p ( α , β ) ( f ; q ; x ) f ( x ) | = | k = 0 n + p ( f ( [ k ] + α [ n ] + β b n ) f ( x ) ) [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) | k = 0 n + p | f ( [ k ] + α [ n ] + β b n ) f ( x ) | [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) M k = 0 n + p | [ k ] + α [ n ] + β b n x | γ [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) .

Using Hölder’s inequality with p= 2 γ and q= 2 2 γ , we get by the statement (2.2)

| C n , p ( α , β ) ( f ; q ; x ) f ( x ) | M k = 0 n + p { [ ( [ k ] + α [ n ] + β b n x ) 2 [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) ] γ 2 × [ [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) ] 2 γ 2 } M [ { k = 0 n + p [ ( [ k ] + α [ n ] + β b n x ) 2 [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) ] } γ 2 × { k = 0 n + p [ [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) ] } 2 γ γ ] = M [ C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) ] γ 2 M ( λ n , q ( x ) ) γ 2 .

 □

Now we give the rate of convergence of the operators by means of the modulus of continuity which is denoted by ω(f;δ). Let f C B [0,) and x0. Then the definition of the modulus of continuity of f is given by

ω(f;δ)= max | t x | δ t , x [ 0 , ) | f ( t ) f ( x ) | .
(4.1)

It follows that for any δ>0 the inequality

|f(x)f(y)|ω(f;δ) ( | x y | δ + 1 )
(4.2)

is satisfied [24].

Theorem 4.2 If f C B [0,), we have

| C n , p ( α , β ) (f;q;x)f(x)|2ω ( f ; λ n , q ( x ) ) ,

where ω(f;) is modulus of continuity of f which is defined in (4.1) and λ n , q (x) be the same as in Theorem  4.1.

Proof By the triangular inequality, we get

| C n , p ( α , β ) ( f ; q ; x ) f ( x ) | = | k = 0 n + p f ( [ k ] + α [ n ] + β b n ) [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) f ( x ) | k = 0 n + p | f ( [ k ] + α [ n ] + β b n ) f ( x ) | [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) .

Now using (4.2) and the Hölder inequality, we can write

| C n , p ( α , β ) ( f ; q ; x ) f ( x ) | k = 0 n + p ( | [ k ] + α [ n ] + β b n x | λ + 1 ) ω ( f ; λ ) [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) = ω ( f ; λ ) k = 0 n + p [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) + ω ( f ; λ ) λ k = 0 n + p | [ k ] + α [ n ] + β b n x | [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) = ω ( f ; λ ) + ω ( f ; λ ) λ { k = 0 n + p ( [ k ] + α [ n ] + β b n x ) 2 [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) } 1 / 2 = ω ( f ; λ ) + ω ( f ; λ ) λ { C n , p ( α , β ) ( ( t x ) 2 ) ; q ; x } 1 / 2 .

Now choosing λ n , q (x) the same as in Theorem 4.1, we have

| C n , p ( α , β ) (f;q;x)f(x)|2ω ( f ; λ n , q ( x ) ) .

 □

Now, we compute the rate of convergence of the operators C n , p ( α , β ) in terms of the modulus of continuity of the derivative of the function.

Theorem 4.3 If f(x) has a continuous bounded derivative f (x) and ω( f ;δ) is the modulus of continuity of f (x) in [0,A], then

| f ( x ) C n , p ( α , β ) ( f ; q ; x ) | M ( | [ n + p ] [ n ] + β 1 | A + α b n [ n ] + β ) + 2 ( B n , q ( α , β ) ) 1 / 2 ω ( f ; ( B n , q ( α , β ) ) 1 / 2 ) ,

where M is a positive constant such that | f (x)|M.

Proof Using the mean value theorem, we have

f ( [ k ] + α [ n ] + β b n ) f ( x ) = ( [ k ] + α [ n ] + β b n x ) f ( ξ ) = ( [ k ] + α [ n ] + β b n x ) f ( x ) + ( [ k ] + α [ n ] + β b n x ) ( f ( ξ ) f ( x ) ) ,

where ξ is a point between x and [ k ] + α [ n ] + β b n . By using the above identity, we get

C n , p ( α , β ) ( f ; q ; x ) f ( x ) = f ( x ) k = 0 n + p ( [ k ] + α [ n ] + β b n x ) [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) + k = 0 n + p ( [ k ] + α [ n ] + β b n x ) ( f ( ξ ) f ( x ) ) [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) .

Hence,

| C n , p ( α , β ) ( f ; q ; x ) f ( x ) | | f ( x ) | | C n , p ( α , β ) ( ( t x ) ; q ; x ) | + k = 0 n + p | [ k ] + α [ n ] + β b n x | | f ( ξ ) f ( x ) | [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) M ( | [ n + p ] [ n ] + β 1 | A + α b n [ n ] + β ) + k = 0 n + p | [ k ] + α [ n ] + β x | | f ( ξ ) f ( x ) | [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) M ( | [ n + p ] [ n ] + β 1 | A + α b n [ n ] + β ) + k = 0 n + p ω ( f ; δ ) ( | [ k ] + α [ n ] + β b n x | δ + 1 ) | [ k ] + α [ n ] + β b n x | [ n + p k ] ( x b n ) k × s = 0 n + p k 1 ( 1 q s x b n ) ,

since

|ξx|| [ k ] + α [ n ] + β b n x|.

Using the above inequality, we have

| C n , p ( α , β ) ( f ; q ; x ) f ( x ) | M ( | [ n + p ] [ n ] + β 1 | A + α b n [ n ] + β ) + ω ( f ; δ ) k = 0 n + p | [ k ] + α [ n ] + β b n x | [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) + ω ( f ; δ ) δ k = 0 n + p ( [ k ] + α [ n ] + β b n x ) 2 [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) .

Therefore, applying the Cauchy-Schwarz inequality for the second term, we get

| C n , p ( α , β ) ( f ; q ; x ) f ( x ) | M ( | [ n + p ] [ n ] + β 1 | A + α b n [ n ] + β ) + ω ( f ; δ ) ( k = 0 n + p ( [ k ] + α [ n ] + β b n x ) 2 [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) ) 1 / 2 + ω ( f ; δ ) δ k = 0 n + p ( [ k ] + α [ n ] + β b n x ) 2 [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) = M ( | [ n + p ] [ n ] + β 1 | A + α b n [ n ] + β ) + ω ( f ; δ ) C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) + ω ( f ; δ ) δ C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) .

Therefore, using (2.2) we see that

sup 0 x A C n , p ( α , β ) ( ( t x ) 2 ; q ; x ) sup 0 x A ( q n [ p ] β ) 2 ( [ n ] + β ) 2 x 2 + ( ( 2 α + 1 ) [ n + p ] ( [ n ] + β ) 2 2 α [ n ] + β ) b n x + α 2 b n 2 ( [ n ] + β ) 2 ( q n [ p ] β ) 2 ( [ n ] + β ) 2 A 2 + | ( 2 α + 1 ) [ n + p ] ( [ n ] + β ) 2 2 α [ n ] + β | A b n + α 2 b n 2 ( [ n ] + β ) 2 : = B n , q ( α , β ) .

Thus,

| C n , p ( α , β ) ( f ; q ; x ) f ( x ) | M ( | [ n + p ] [ n ] + β 1 | A + α b n [ n ] + β ) + ω ( f ; δ ) [ ( B n , q ( α , β ) ) 1 / 2 + 1 δ B n , q ( α , β ) ] .

Choosing δ:= δ n , q (p)= ( B n , q ( α , β ) ) 1 / 2 , we obtain the desired result. □

5 Generalization of the Chlodowsky variant of q-Bernstein-Schurer-Stancu operators

In this section, we introduce generalization of Chlodowsky variant of q-Bernstein-Schurer-Stancu operators. The generalized operators help us to approximate the continuous functions on more general weighted spaces. Note that this kind of generalization was considered earlier for the Bernstein-Chlodowsky polynomials [22] and q-Bernstein-Chlodowsky polynomials [25].

For x0, consider any continuous function ω(x)1 and define

G f (t)=f(t) 1 + t 2 ω ( t ) .

Let us take into account the generalization of the C n , p ( α , β ) (f;q;x) as follows:

L n , p α , β (f;q;x)= ω ( x ) 1 + x 2 k = 0 n + p G f ( [ k ] + α [ n ] + β b n ) [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) ,

where 0x b n and ( b n ) has the same properties as the Chlodowsky variant of the q-Bernstein-Schurer-Stancu operators.

Theorem 5.1 For the continuous functions satisfying

lim x f ( x ) ω ( x ) = K f <,

we have

lim n sup 0 x b n | L n , p α , β ( f ; q ; x ) f ( x ) | ω ( x ) =0.

Proof Clearly,

L n , p α , β ( f ; q ; x ) f ( x ) = ω ( x ) 1 + x 2 ( k = 0 n + p G f ( [ k ] + α [ n ] + β b n ) [ n + p k ] ( x b n ) k s = 0 n + p k 1 ( 1 q s x b n ) G f ( x ) ) ,

thus

sup 0 x b n | L n , p α , β ( f ; q ; x ) f ( x ) | ω ( x ) = sup 0 x b n | C n , p ( α , β ) ( G f ; q ; x ) G f ( x ) | 1 + x 2 .

By using |f(x)| M f ω(x) and continuity of the function f, we get | G f (x)| M f (1+ x 2 ) for x0 and G f (x) is continuous function on [0,). Thus, from Theorem 3.2 we get the result. □

Finally note that, taking ω(x)=1+ x 2 , the operators L n , p α , β (f;q;x) reduce to C n , p ( α , β ) ( G f ;q;x).

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Vedi, T., Ali Özarslan, M. Chlodowsky variant of q-Bernstein-Schurer-Stancu operators. J Inequal Appl 2014, 189 (2014). https://doi.org/10.1186/1029-242X-2014-189

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