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Article

Genuine q-Stancu-Bernstein–Durrmeyer Operators

by
Pembe Sabancıgil
Department of Mathematics, Faculty of Arts and Sciences, Eastern Mediterranean University, Gazimagusa 99628, Cyprus
Symmetry 2023, 15(2), 437; https://doi.org/10.3390/sym15020437
Submission received: 10 January 2023 / Revised: 24 January 2023 / Accepted: 30 January 2023 / Published: 7 February 2023

Abstract

:
In the present paper, we introduce the genuine q-Stancu-Bernstein–Durrmeyer operators Z n q , α ( f ; x ) . We calculate the moments of these operators, Z n q , α ( t j ; x ) for j = 0 , 1 , 2 , which follows a symmetric pattern. We also calculate the second order central moment Z n q , α ( ( t x ) 2 ; x ) . We give a Korovkin-type theorem; we estimate the rate of convergence for continuous functions. Furthermore, we prove a local approximation theorem in terms of second modulus of continuity; we obtain a local direct estimate for the genuine q-Stancu-Bernstein–Durrmeyer operators in terms of Lipschitz-type maximal function of order β and we prove a direct global approximation theorem by using the Ditzian-Totik modulus of second order.

1. Introduction

A sequence of positive linear operators S n ( α ) : C [ 0 , 1 ] C [ 0 , 1 ] was introduced and studied by a Romanian mathematician D.D. Stancu [1] in 1968. The operators depend on a non-negative parameter α and are defined as follows:
S n ( α ) ( f , x ) = k = 0 n f k n p n , k ( α ) x ,
where p n , k ( α ) x is the Polya distribution with density function given by
p n , k ( α ) x = n k i = 0 k 1 ( x + i α ) s = 0 n k 1 ( 1 x + s α ) i = 0 n 1 ( 1 + i α ) , x [ 0 , 1 ] .
If α = 0 , the operators S n ( α ) reduce to the well-known classical Bernstein polynomials. A. Lupaş and L. Lupaş [2] studied on a particular case for Stancu’s operators by setting α = 1 n and obtained
S n ( 1 n ) ( f , x ) = 2 ( n ! ) ( 2 n ! ) k = 0 n n k f k n ( n x ) k ( n n x ) n k ,
where ( y ) n = y ( y + 1 ) ( y + 2 ) ( y + n 1 ) is the rising factorial with ( y ) 0 = 1 .
For any function f C [ 0 , 1 ] , α 0 , q > 0 and each n N , modification of the Stancu’s operators based on the q-integers is introduced by G. Nowak [3] in 2009 as follows:
B n q , α ( f , x ) = k = 0 n p n , k q , α x f [ k ] q [ n ] q x [ 0 , 1 ] ,
where
p n , k q , α x = n k q i = 0 k 1 ( x + α i q ) s = 0 n k 1 ( 1 q s x + α [ s ] q ) i = 0 n 1 ( 1 + α i q ) ,
p n , k q , α 1 = 0 , p n , n q , α 1 = 1 , s = 0 1 ( ) = 1 .
G. Nowak studied the Korovkin type approximation properties for the q-analogue of the Stancu’s operators B n q , α ( f , x ) . If α = 0 ,   B n q , α ( f , x ) reduces to the q-Bernstein polynomials defined by GM. Phillips in [4] as
B n , q f , x = k = 0 n f k q n q p n k ( q ; x ) ,
where
p n , k q , x : = n k q x k s = 0 n k 1 ( 1 q s x ) .
For q 1 , they reduce to Bernstein-Stancu operators. For α = 0 and q 1 , they reduce to the classical Bernstein polynomials.
On the other hand, integral modification of classical Bernstein polynomials was introduced by J.L. Durrmeyer ([5]) in 1967. This type of modification was studied in several forms by different authors (see [6,7,8,9] and etc.). Classical genuine Bernstein-Durrmeyer operators were independently introduced by W. Chen ([10]) in 1987, and by T. N. T. Goodman & A. Sharma ([11]) later in 1991 and these operators were investigated by many authors, see for example [12,13]. They possess many interesting properties, in particular they reproduce linear functions and thus interpolate every function f C [ 0 , 1 ] at x = 0 and x = 1 . V. Gupta ([14]) introduced the q-analogue of the Bernstein–Durrmeyer operators and studied some approximation properties for these operators.
To approximate continuous functions, V. Gupta and H. Wang ([15]) defined the q-Durrmeyer type operators as
M n , q ( f , x ) : = f ( 0 ) p n , 0 ( q , x ) + [ n + 1 ] q k = 1 n q 1 k p n , k q ; x 0 1 p n , k 1 q ; q t f t d q t
and they studied estimation of the rate of convergence for continuous functions in terms of modulus of continuity. N. Mahmudov and P. Sabancıgil ([16]) defined and studied genuine q-Bernstein-Durrmeyer operators. T. Neer, P.N. Agrawal and S. Araci ([17]) constructed the Stancu-Durrmeyer type modification of q-Bernstein operators by means of q-Jackson integral. V. Gupta and Z. Finta ([18]) studied some direct local and global approximation theorems for the q-Durrmeyer operators for 0 < q < 1 . In [19,20] P. Sabancıgil shortly mentioned about some parts of the q-Stancu-Bernstein–Durrmeyer operators. Also, the rapid rise of post quantum calculus or shortly ( p , q ) -calculus has led to the discovery of new generalizations of this type of operators based on ( p , q ) -integers. M. Mursaleen et al. studied on ( p , q ) -analogue of Bernstein operators, some approximation results by ( p , q ) -analogue of Bernstein Stancu operators, approximation by ( p , q ) -Baskakov-Durrmeyer-Stancu operators, bivariate Bernstein-Schurer-Stancu type GBS operators in ( p , q ) -analogue and etc. (see [21,22,23,24]). Q.B. Chai and G. Zhou studied on ( p , q ) -analogue of Kantorovich type Bernstein-Stancu-Schurer operators (see [25]). V.N. Mishra studied Baskakov-Durrmeyer-Stancu operators (see [26]). I. Yuksel, U.D. Kantar and B. Altın studied on the ( p , q ) -Stancu generalization of a genuine Baskakov-Durrmeyer type operators (see [27]).
q-Stancu-Durrmeyer operators defined by T. Neer, P.N. Agrawal and S. Araci ([17]) do not preserve linear functions. The main motivation of this paper is to construct a q-analogue of Stancu-Bernstein–Durrmeyer type operators, Z n q , α ( f ; x ) , which preserves linear functions, i.e., Z n q , α ( e 0 ; x ) = e 0 ( x ) and Z n q , α ( e 1 ; x ) = e 1 ( x ) for e i ( x ) = x i ( i = 0 , 1 ) and interpolate every function f C [ 0 , 1 ] at x = 0 and x = 1 .
In this paper, we introduce genuine q-Stancu-Bernstein–Durrmeyer Operators Z n q , α in detail. We calculate the moments of these operators Z n q , α ( t j ; x ) for j = 0 , 1 , 2 and observe that they follow a symmetrical pattern. We calculate the second order central moment Z n q , α ( ( t x ) 2 ; x ) . We examine convergence properties of the operators, estimate the rate of convergence and we prove a Korovkin-type theorem. We also present a local approximation theorem by using the second order modulus of smoothness, we provide a local direct estimate in terms of Lipschitz type maximal function of order β and we offer a global approximation theorem by using Ditzian-Totik modulus of second order. Compared to the previous generalizations of this type of operator, the advantage of genuine q-Stancu-Bernstein–Durrmeyer operators is that they reproduce linear functions and they interpolate every function f C [ 0 , 1 ] at x = 0 and x = 1 , i.e., Z n q , α ( f ; 0 ) = f ( 0 ) and Z n q , α ( f ; 1 ) = f ( 1 ) .
First of all, we provide some notations and definitions of q-integers:
Let 0 < q < 1 . For any n N 0 , the q-integer n q is defined by
n q : = 1 + q + + q n 1 , 0 q : = 0 ;
and the q-factorial n q ! by
n q ! : = 1 q 2 q n q , 0 q ! : = 1 .
For integers 0 k n , the q-binomial is defined by
n k q : = n q ! k q ! n k q ! .
The q-analogue of integration in the interval [ 0 , A ] (see [28]) is defined by
0 A f t d q t : = A 1 q n = 0 f A q n q n , 0 < q < 1 .
For more information on q-calculus one can see [28].
The paper is organized as follows: In Section 2, we calculate the moments of these operators Z n q , α ( t j ; x ) for j = 0 , 1 , 2 and the second order central moment Z n q , α ( ( t x ) 2 ; x ) , we show that Z n q , α t m ; x is a polynomial of degree less than or equal to min m , n and we prove that for f C [ 0 , 1 ] and 0 < q < 1 , Z n q , α f ; x = f ( x ) for all x [ 0 , 1 ] if and only if f is linear. In Section 3, we examine convergence properties of the operators. In Section 4, we give an estimation for the rate of convergence, we prove a local approximation theorem by using the second order modulus of smoothness, we obtain a local direct estimate in terms of Lipschitz type maximal function of order β and we prove a global approximation theorem by using second order Ditzian-Totik modulus. In Section 5, we present conclusions and suggest further studies.

2. Operators and Estimation of Their Moments

Definition 1.
For f C 0 , 1 , α 0 and 0 < q < 1 , we define the following genuine q-Stancu-Bernstein–Durrmeyer Operators:
Z n q , α f ; x = p n , 0 q , α ( x ) f ( 0 ) + p n , n q , α ( x ) f ( 1 ) + n 1 q k = 1 n 1 q 1 k p n , k q , α ( x ) 0 1 p n 2 , k 1 ( q ; q t ) f ( t ) d q t . ,
where for n = 1 the sum is empty, i.e., equal to 0 ,
p n , k q , α x = n k q i = 0 k 1 ( x + α i q ) s = 0 n k 1 ( 1 q s x + α [ s ] q ) i = 0 n 1 ( 1 + α i q ) ,
p n , k q , α 1 = 0 , p n , n q , α 1 = 1 , s = 0 1 ( ) = 1 ,
and
p n , k q , x : = n k q x k s = 0 n k 1 ( 1 q s x ) .
Moments and central moments play an important role in approximation theory. In the following lemma, we obtain explicit formulas for Z n q , α t m ; x for m = 0 , 1 , 2 and Z n q , α t x 2 ; x .
Lemma 1.
We have
Z n q , α 1 ; x = 1 , Z n q , α t ; x = x , Z n q , α t 2 ; x = 1 [ n + 1 ] q x + q [ n ] q [ n + 1 ] q 1 1 + α x ( x + α ) + x ( 1 x ) n q , Z n q , α t x 2 ; x = α 1 + α + 1 + q [ n + 1 ] q ( 1 + α ) x ( 1 x ) .
Proof. 
By using the definition of q-Beta function (see [28]), we have the following equalities for r = 0 , 1 ,
0 1 t r p n 2 , k 1 q ; q t d q t = n 2 k 1 q q k 1 0 1 t k + r 1 r = 0 n k 2 ( 1 q r + 1 t ) d q t = q k 1 n 2 q ! k 1 q ! n 1 k q ! k + r 1 q ! n 1 k q ! n + r 1 q ! = q k 1 n 2 q ! k + r 1 q ! k 1 q ! n + r 1 q ! .
We are going to use the following identities for the proof of the theorem (see [3]):
k = 0 n p n , k q , α x = 1 , k = 0 n p n , k q , α x k q n q = x , k = 0 n p n , k q , α x k q 2 n q 2 = 1 1 + α x ( x + α ) + x ( 1 x ) n q .
Using Definition 1 and equality (1) and by using the above identities, we have
Z n q , α 1 ; x = p n , 0 q , α ( x ) + p n , n q , α ( x ) + n 1 q k = 1 n 1 q 1 k p n , k q , α ( x ) 0 1 p n 2 , k 1 ( q ; q t ) d q t = p n , 0 q , α ( x ) + p n , n q , α ( x ) + n 1 q k = 1 n 1 q 1 k p n , k q , α ( x ) q k 1 n 1 q = p n , 0 q , α ( x ) + p n , n q , α ( x ) + k = 1 n 1 p n , k q , α ( x ) = k = 0 n p n , k q , α ( x ) = 1 .
Z n q , α t ; x = p n , n q , α ( x ) + n 1 q k = 1 n 1 q 1 k p n , k q , α ( x ) 0 1 t p n 2 , k 1 ( q ; q t ) d q t = p n , n q , α ( x ) + n 1 q k = 1 n 1 q 1 k p n , k q , α ( x ) q k 1 [ k ] q [ n 1 ] q [ n ] q = p n , n q , α ( x ) + k = 1 n 1 p n , k q , α ( x ) [ k ] q [ n ] q = k = 0 n p n , k q , α ( x ) [ k ] q [ n ] q = x
and
Z n q , α t 2 ; x = p n , n q , α x + n 1 q k = 1 n 1 q 1 k p n , k q , α x 0 1 t 2 p n 2 , k 1 q ; q t d q t = p n , n q , α x + n 1 q k = 1 n 1 q 1 k p n , k q , α x q k 1 n 2 q ! k + 1 q ! k 1 q ! n + 1 q ! = p n , n q , α x + 1 n + 1 q k = 1 n 1 p n , k q , α x k q ( q k q + 1 ) n q = p n , n q , α x + 1 n + 1 q k = 0 n 1 p n , k q , α x k q n q + q n q n + 1 q k = 0 n 1 p n , k q , α x k q 2 n q 2 = p n , n q , α x + 1 n + 1 q x p n , n q , α x + q n q n + 1 q 1 1 + α x ( x + α ) + x ( 1 x ) n q p n , n q , α x = 1 n + 1 q x + q n q n + 1 q 1 1 + α x ( x + α ) + x ( 1 x ) n q .
Now, for the proof of Z n q , α ( t x ) 2 ; x , we use Z n q , α t 2 ; x and the linearity of the operators as follows:
Z n q , α ( t x ) 2 ; x = Z n q , α ( t 2 2 x t + x 2 ) ; x = Z n q , α t 2 ; x 2 x Z n q , α t ; x + x 2 = Z n q , α t 2 ; x x 2 = 1 [ n + 1 ] q x + q [ n ] q [ n + 1 ] q 1 1 + α x ( x + α ) + x ( 1 x ) n q x 2 = 1 q [ n ] q [ n + 1 ] q 1 1 + α x ( 1 x ) + q [ n + 1 ] q 1 1 + α x ( 1 x ) + x 1 + α + q [ n ] q ( α + 1 ) [ n + 1 ] q ( 1 + α ) 1 = 1 q [ n ] q [ n + 1 ] q 1 1 + α x ( 1 x ) + q [ n + 1 ] q 1 1 + α x ( 1 x ) = [ n + 1 ] q + α [ n + 1 ] q [ n + 1 ] q 1 + q [ n + 1 ] q 1 1 + α x ( 1 x ) = α [ n + 1 ] q + 1 + q [ n + 1 ] q 1 1 + α x ( 1 x ) = α 1 + α + 1 + q [ n + 1 ] q ( 1 + α ) x ( 1 x ) .
Lemma is proved. □
Lemma 2.
Z n q , α t m ; x is a polynomial of degree less than or equal to min m , n .
Proof. 
By using simple calculations, we obtain
Z n q , α t m ; x = n 1 q k = 1 n 1 q 1 k p n , k q , α x 0 1 p n 2 , k 1 q ; q t t m d q t + p n , n q , α x = n 1 q k = 1 n 1 p n , k q , α x n 2 q ! k + m 1 q ! k 1 q ! n + m 1 q ! + p n , n q , α x = n 1 q ! n + m 1 q ! k = 1 n 1 p n , k q , α x k + m 1 q ! k 1 q ! + p n , n q , α x = n 1 q ! n + m 1 q ! k = 1 n 1 k q k + 1 q k + m 1 q p n , k q , α x + p n , n q , α x = n 1 q ! n + m 1 q ! k = 1 n k q k + 1 q k + m 1 q p n , k q , α x .
Now using the identity that
k q k + 1 q k + m 1 q = j = 0 m 1 q j k q + j q = j = 1 m c j m k q j ,
where c j m > 0 , j = 1 , 2 , , m , are the constants independent of k, we get
Z n q , α t m ; x = n 1 q ! n + m 1 q ! k = 1 n j = 1 m c j m k q j p n , k α q ; x = n 1 q ! n + m 1 q ! j = 1 m c j m n q j B n , q α t j ; x .
From [3], we know that B n , q α t j ; x is a polynomial of degree less than or equal to min j , n and c j m > 0 , j = 1 , 2 , , m . Thus it follows that Z n q , α t m ; x is a polynomial of degree less than or equal to min m , n . □
Theorem 1.
Let f C [ 0 , 1 ] and 0 < q < 1 . Then Z n q , α f ; x = f ( x ) for all x [ 0 , 1 ] if and only if f is linear.
Proof. 
From Theorem 9 of [29], we know that for a positive linear operator D on C [ 0 , 1 ] which reproduces linear functions, if D ( t 2 , x ) > x 2 for all x ( 0 , 1 ) , then D ( f ) = f if and only if f is linear. Now, since Z n q , α is a positive linear operator on C [ 0 , 1 ] which reproduces linear functions, it sufficies to show that Z n q , α t 2 ; x > x 2 for all x ( 0 , 1 ) .
Let h ( x ) = Z n q , α t 2 ; x x 2 . One can easily see that h ( 0 ) = h ( 1 ) = 0 . On the other hand we have,
h ( x ) = q n q n + 1 q 2 1 + α q n + 1 q 2 1 + α 2 = 2 q 2 n 1 q n + 1 q 1 1 + α 2 < 0 .
Now since the function h is concave down on ( 0 , 1 ) and h ( 0 ) = h ( 1 ) = 0 , we conclude that h ( x ) > 0 for all x ( 0 , 1 ) which implies that Z n q , α t 2 ; x > x 2 for all x ( 0 , 1 ) . This completes the proof of the theorem. □

3. Convergence of Genuine q-Stancu-Bernstein-Durrmeyer Operators

Theorem 2.
Let ( q n ) and ( α n ) be two sequences such that 0 < q n 1 and α n 0 . Then the sequence Z n q n , α n f converges to f uniformly on 0 , 1 for each f C 0 , 1 if and only if lim n q n = 1 and lim n α n = 0 .
Proof. 
From the definition of Z n q , α f and Lemma 1 it follows that the operators Z n q n , α n are positive linear operators on C 0 , 1 and reproduce linear functions. The well-known Korovkin theorem implies that Z n q n , α n f converges to f ( x ) uniformly on [ 0 , 1 ] as n for any f C 0 , 1 if and only if
Z n q n , α n t 2 ; x x 2
uniformly on [ 0 , 1 ] as n . If q n 1 ( [ n ] q n ) and α n 0 then (2) follows from Lemma 1.
On the other hand, if we assume that for any f C 0 , 1 , Z n q n , α n f converges to f ( x ) uniformly on [ 0 , 1 ] as n , then Z n q n , α n t 2 ; x x 2 . Hence
1 [ n + 1 ] q n x + q n [ n ] q n [ n + 1 ] q n 1 1 + α n x ( x + α n ) + x ( 1 x ) n q n x 2 .
Consequently
q n [ n ] q n [ n + 1 ] q n 1 1 + α n 1 1 [ n ] q n x 2 + 1 [ n + 1 ] q n + q n [ n ] q n [ n + 1 ] q n α n 1 + α n + q n [ n + 1 ] q n 1 1 + α n x
converges to x 2 . Therefore
q n [ n ] q n [ n + 1 ] q n 1 1 + α n 1 1 [ n ] q n 1 and 1 [ n + 1 ] q n + q n [ n ] q n [ n + 1 ] q n α n 1 + α n + q n [ n + 1 ] q n 1 1 + α n 0 .
Since α n and [ n ] q n are both nonnegative we get α n 0 and [ n ] q n ( q n 1 ), which completes the proof of the theorem. □
Lemma 3.
For f C [ 0 , 1 ] , we have Z n q , α f f .
Proof. 
From Definition 1 and from Lemma 1, we have
Z n q , α f ; x f ( 0 ) p n , 0 q , α x + f ( 1 ) p n , n q , α x + n 1 q k = 1 n 1 q 1 k p n , k q , α x 0 1 p n 2 , k 1 q ; q t f t d q t f Z n q , α 1 ; x = f .

4. Approximation Properties of q-Stancu-Bernstein–Durrmeyer Operators

We consider the following K-functional:
K 2 f , δ 2 : = inf f h + δ 2 h : h C 2 0 , 1 , δ 0 ,
where the space C 2 0 , 1 is defined as
C 2 0 , 1 : = h : h , h , h C 0 , 1 .
Then, from the well known result in [30], there exists an absolute constant C 1 > 0 such that
K 2 f , δ 2 C 1 ω 2 f , δ
where
ω 2 f , δ : = sup 0 < y δ sup x ± y 0 , 1 f x y 2 f x + f x + y
is the second modulus of smoothness of f C 0 , 1 .
In the following theorem, we state our first main result for this section. We prove a local approximation theorem for the genuine q-Stancu-Bernstein–Durrmeyer Operators Z n q , α .
Theorem 3.
There exists an absolute constant L > 0 such that
Z n q , α f ; x f x L ω 2 f , α 1 + α + 1 + q [ n + 1 ] q ( 1 + α ) x 1 x ,
where f C [ 0 , 1 ] , 0 < q < 1 .
Proof. 
Using the Taylor formula
h t = h x + h x t x + x t t s h s d s , h C 2 0 , 1 ,
we obtain that
Z n q , α h ; x = h x + Z n q , α x t t s h s d s ; x , h C 2 [ 0 , 1 ] .
It is obvious that x t t s h s d s h t x 2 . Hence
Z n q , α h ; x h x Z n q , α x t t s . h s d s ; x h Z n q , α t x 2 ; x = h α 1 + α + 1 + q [ n + 1 ] q ( 1 + α ) x ( 1 x ) .
Now for f C 0 , 1 and h C 2 0 , 1 we obtain
Z n q , α f ; x f x Z n q , α f h ; x + Z n q , α h ; x h x + f x h x 2 f h + h α 1 + α + 1 + q [ n + 1 ] q ( 1 + α ) x ( 1 x ) .
Taking the infimum on the right hand side over all h C 2 0 , 1 , we obtain
Z n q , α f ; x f x 2 K 2 f , α 1 + α + 1 + q [ n + 1 ] q ( 1 + α ) x 1 x .
Now the desired inequality follows from (3) and (4). □
We know that a function f C [ 0 , 1 ] belongs to the Lipschitz type space L i p M ( β ) , ( M > 0 and 0 < β 1 ), provided that
f ( t ) f ( x ) M t x β , for all x , t [ 0 , 1 ] .
Then we have the following result.
Theorem 4.
Let x [ 0 , 1 ] . Then, for all f L i p M ( β ) , n N , α 0 and 0 < q < 1 , we have
Z n q , α ( f ; x ) f ( x ) M λ α , n ( x , q ) β 2 ,
where
λ α , n ( x , q ) = α 1 + α + 1 + q [ n + 1 ] q ( 1 + α ) x ( 1 x ) ,
M is a constant depending on β and f .
Proof. 
Let f L i p M ( β ) , 0 < β 1 . By (5), we may write
Z n q , α ( f ; x ) f ( x ) Z n q , α f ( t ) f ( x ) ; x M Z n q , α t x β .
Now, applying the Hölder inequality with p = 2 β and q = 2 2 β , we get
Z n q , α ( f ; x ) f ( x ) M Z n q , α t x β p ; x 1 p Z n q , α 1 q ; x 1 q = M Z n q , α t x 2 ; x β 2 = M α 1 + α + 1 + q [ n + 1 ] q ( 1 + α ) x ( 1 x ) β 2 = M λ α , n ( x , q ) β 2
and the proof is completed. □
In the next theorem, we give the direct global approximation theorem for the genuine q-Stancu-Bernstein–Durrmeyer Operators Z n q , α . Before stating the theorem we recall the weighted K-functional of second order for f C [ 0 , 1 ] , it is defined by
K 2 , ϕ f , δ 2 : = inf f g + δ 2 ϕ 2 g : g W 2 ϕ , δ 0 , ϕ 2 = x 1 x
where
W 2 ϕ : = g C 0 , 1 : g A C l o c 0 , 1 , ϕ 2 g C 0 , 1 ,
and g A C l o c 0 , 1 means that g is differentiable and g is absolutely continuous in every closed interval a , b 0 , 1 . Furthermore, the Ditzian-Totik modulus of second order is given by
ω 2 ϕ f , δ : = sup 0 < g δ sup x ± g ϕ x [ 0 , 1 ] f x ϕ x g 2 f x + f x + ϕ x g .
It is well known that K-functional K 2 , ϕ f , δ 2 and Ditzian-Totik modulus ω 2 ϕ f , δ are equivalent, see [30].
Theorem 5.
Let f C [ 0 , 1 ] , 0 < q < 1 . There exists an absolute constant L > 0 such that
Z n q , α f f L ω 2 ϕ f , α 1 + α + 1 [ n + 1 ] q ( 1 + α ) .
Proof. 
From the Taylor expansion, we can write
h t = h x + h x t x + x t x p h s d s d p .
Now, applying Z n q , α to both sides of the last equation we get
Z n q , α h ; x h x Z n q , α x t x p h s d s d p ; x ϕ 2 h Z n q , α x t x p 1 ϕ 2 s d s d p ; x ϕ 2 h Z n q , α x t t s ϕ 2 s d s ; x .
Let s = t + p x t , p 0 , 1 . Using the concavity of ϕ 2 we have
t s ϕ 2 s = p x t ϕ 2 t + p x t p x t ϕ 2 t + p ϕ 2 x ϕ 2 t x t ϕ 2 x .
Therefore
x t t s ϕ 2 s d s x t x t ϕ 2 x d s = t x 2 ϕ 2 x
and
Z n q , α h ; x h x ϕ 2 h 1 ϕ 2 x Z n q , α t x 2 ; x .
Since Z n q , α is a bounded operator, we obtain for f C 0 , 1 that
Z n q , α f ; x f x Z n q , α f h ; x + Z n q , α h ; x h x + f x h x 2 f h + ϕ 2 h α 1 + α + 1 + q [ n + 1 ] q ( 1 + α ) .
Now, if we take the infimum on the right hand side over all h with h A C l o c [ 0 , 1 ] we obtain
Z n q , α f ; x f x 2 K 2 , ϕ f , α 1 + α + 1 [ n + 1 ] q ( 1 + α ) .
Finally, from the fact that K 2 , ϕ ( f , δ 2 ) and ω ϕ 2 f , δ are equivalent we obtain the desired result. □

5. Conclusions

Inspired from the previous studies, our goal was to construct a generalization of Stancu-Bernstein–Durrmeyer type operators based on the q-integers which reproduces linear functions and interpolates every function f C [ 0 , 1 ] at x = 0 and x = 1 .
In this paper, by using the q-analogue of integers, we defined the genuine q-Stancu-Bernstein–Durrmeyer Operators Z n q , α f ; x . We gave explicit formulas for the moments of these operators Z n q , α ( t j ; x ) for j = 0 , 1 , 2 and for the second order central moment Z n q , α ( ( t x ) 2 ; x ) . We proved a Korovkin-type theorem and we provided an estimation of the rate of convergence for these operators. We proved a local approximation theorem by using the second order modulus of smoothness, we obtained a local direct estimate in terms of Lipschitz-type maximal function of order β and we proved a global approximation theorem by using Ditzian-Totik modulus of second order. The newly defined genuine q-Stancu-Bernstein–Durrmeyer operators have some advantages compared to the similar generalizations of this type of operator which was defined before. The advantage of genuine q-Stancu-Bernstein–Durrmeyer operators is that they preserve linear functions, i.e., Z n q , α ( e 0 ; x ) = e 0 ( x ) and Z n q , α ( e 1 ; x ) = e 1 ( x ) for e i ( x ) = x i ( i = 0 , 1 ) and furthermore, they interpolate every function f C [ 0 , 1 ] at x = 0 and x = 1 , i.e., Z n q , α ( f ; 0 ) = f ( 0 ) and Z n q , α ( f ; 1 ) = f ( 1 ) . As a future work we would like to construct genuine ( p , q ) -Stancu-Bernstein–Durrmeyer operators Z n p , q , α f ; x by using the theory of post quantum calculus and examine their approximation properties.

Funding

This research received no external funding.

Data Availability Statement

Not applicable.

Acknowledgments

The author would like to express her sincere thanks to the editor and the anonymous reviewers for their valuable comments and suggestions.

Conflicts of Interest

The authors declare no conflict to interest.

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Sabancıgil, P. Genuine q-Stancu-Bernstein–Durrmeyer Operators. Symmetry 2023, 15, 437. https://doi.org/10.3390/sym15020437

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Sabancıgil P. Genuine q-Stancu-Bernstein–Durrmeyer Operators. Symmetry. 2023; 15(2):437. https://doi.org/10.3390/sym15020437

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Sabancıgil, Pembe. 2023. "Genuine q-Stancu-Bernstein–Durrmeyer Operators" Symmetry 15, no. 2: 437. https://doi.org/10.3390/sym15020437

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