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Approximation Properties of Chlodovsky Type Two Dimensional Bernstein Operators Based on (p, q)−integers

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28 October 2024

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04 November 2024

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Abstract
In this paper, we present two-dimensional Chlodovsky-type Bernstein operators constructed using (p, q)−integers, and evaluate their approximation properties within the framework of a Korovkin-type theorem. Our investigation extends to local approximation properties, with a focus on determining convergence rates via the modulus of continuity and a Lipschitz-type maximal function. A Voronovskaja-type theorem is also derived, offering insight into the asymptotic behavior of these operators. Additionally, we explore weighted approximation properties and analyze convergence rates within specific function spaces. Utilizing Maple for visual representations, we demonstrate the efficiency of these operators in approximating specific functions. The practical implications of these findings extend to the optimization of system control, improving the stability and performance of dynamic systems. Our contributions also offer new perspectives on the application of approximation methods in fractional differential equations and control theory, broadening the scope of their use in mathematical modeling.
Keywords: 
Subject: 
Computer Science and Mathematics  -   Analysis

1. Introduction

The study provides a comprehensive examination of the theory and applications of mathematical operators, aligning with the content areas of Mathematics, Engineering, Physics, and Computer Science. The investigation of the convergence properties of Chlodovsky type Bernstein operators using the Korovkin-type theorem is directly part of mathematical analysis and approximation theory. Such studies yield significant results applicable to fields like mathematical modeling and optimization. Furthermore, the optimization of convergence rates of operators through system control contributes to the more efficient and stable management of systems within control engineering. Lastly, visual illustrations created using Maple demonstrate the convergence rates of operators on specific functions, contributing to modeling and simulation techniques used in computer science. In this context, our work offers a valuable addition to the scope of the journal Symmetry.
Approximation theory is rapidly emerging as an essential tool, extending its influence beyond classical domains to other mathematical areas such as differential equations, orthogonal polynomials, and geometric design. Following the introduction of Korovkin’s renowned theorem in 1950, the topic of approximating functions using linear positive operators has become an increasingly significant focus within approximation theory. A wealth of literature has been produced on this subject [1,2,10,12,14,15,23,24,31,32].
In recent years, particularly over the last twenty years, the role of q-calculus in approximation theory has been thoroughly investigated. The initial work on Bernstein polynomials derived from q-integers was conducted by Lupaş [6]. His findings indicated that q-Bernstein polynomials can provide superior approximations compared to classical methods when an appropriate choice of q is made. This discovery has encouraged numerous researchers to develop q-generalizations of various operators and to explore their approximation properties further. Numerous studies have contributed to this field [3,7,8,13].
Lately, Mursaleen et al. have concentrated on utilizing ( p , q ) calculus for approximations through linear positive operators, introducing the ( p , q ) analogues of Bernstein operators [20,21]. They analyzed the uniform convergence of these operators and determined their rates of convergence. For additional recent studies related to ( p , q ) operators, readers can refer to [17,18,19,26,27].
The main motivation behind this study is that, to the authors’ knowledge, there have been no investigations into approximating two-variable operators using ( p , q ) calculus thus far. In this context, we introduce two dimensional Chlodovsky type Bernstein operators based on ( p , q ) integers. We investigate the approximation properties of our newly defined operators with the aid of the Korovkin-type theorem. Furthermore, we delve into the local approximation characteristics and determine the rates of convergence through the modulus of continuity and a Lipschitz type maximal function. A Voronovskaja type theorem relevant to these operators is also presented. Another significant aim of this research is to examine the weighted approximation properties of our operators in the first quadrant of R + 2 , specifically within the range of [ 0 , ) × [ 0 , ) . To achieve these results, we intend to apply a weighted Korovkin-type theorem. We will begin by revisiting some definitions and notations pertinent to the concept of (p, q)-calculus. The (p, q)-integer associated with a given number n is defined as
n p , q : = p n q n p q , n = 1 , 2 , 3 , 0 < q < p 1 .
The ( p , q ) factorial n p , q ! and the ( p , q ) binomial coefficients are defined as:
n p , q ! : = l l n p , q n 1 p , q 1 p , q , n N 1 , n = 0 .
and
n k p , q = n p , q ! k p , q ! n k p , q ! , 0 k n .
Further, the ( p , q ) binomial expansions are given as
( a x + b y ) p , q n = k = 0 n p n k 2 q k 2 a n k b k x n k y k .
and
( x y ) p , q n = ( x y ) ( p x q y ) ( p 2 x q 2 y ) ( p n 1 x q n 1 y ) .
Further information related to ( p , q ) calculus can be found in [25,28].

2. Construction of the Operators

Recently, Ansari and Karaisa [16] have defined and studied ( p , q ) analogue of Chlodovsky operators as follows:
C n , p , q f ; x = 1 p n ( n 1 ) / 2 k = 0 n n k p , q p k ( k 1 ) / 2 x b n k 1 x b n p , q n k 1 f k p , q n p , q p k n b n ,
where
1 x b n p , q n k 1 = s = 0 n k 1 p s q s x b n .
For 0 < q 1 , q 2 < p 1 , p 2 1 , we define Chlodovsky type two dimensional Bernstein operator based on ( p , q ) integers as follows:
C n , m ( p 1 , q 1 ) , ( p 1 , q 1 ) f ; x , y = k = 0 n j = 0 m Φ n , k ( p 1 , q 1 ; x ) Φ m , j ( p 2 , q 2 ; y ) f k p 1 , q 1 n p 1 , q 1 p 1 k n α n , j p 2 , q 2 m p 2 , q 2 p 2 j m β m ,
for all n , m N , f C ( I α n β m ) with I α n β m = { ( x , y ) : 0 α n x , 0 β m y } and C ( I α n β m ) = { f : I α n β m R is continuous } . Here ( α n ) and ( β m ) be increasing unbounded sequences of positive real numbers such that
lim n α n [ n ] p 1 , q 1 = 0 ,
lim m β m [ m ] p 2 , q 2 = 0 .
Also, the basis elements are
Φ n , k ( p 1 , q 1 ; x ) = p 1 k ( k 1 ) n ( n 1 ) 2 n k p 1 , q 1 x α n k s = 0 n k 1 p 1 s q 1 s x α n , Φ m , j ( p 2 , q 2 ; y ) = p 2 j ( j 1 ) m ( m 1 ) 2 m j p 2 , q 2 y β m j s = 0 m j 1 p 2 s q 2 s y β m .
We require the following lemmas to establish our main results.
Lemma 1.
[16]
C n , p , q 1 ; x = 1 , C n , p , q e 1 ; x = x , C n , p , q e 2 ; x = p n 1 b n [ n ] p , q x + q [ n 1 ] p , q [ n ] p , q x 2 C n , p , q e 3 ; x = b n 2 x [ n ] p , q 2 p 2 n 2 + ( 2 p + q ) q [ n 1 ] p , q x 2 b n [ n ] p , q 2 p n 1 + q 3 [ n 1 ] p , q [ n 2 ] p , q x 3 [ n ] p , q 2 , C n , p , q e 4 ; x = b n 3 x [ n ] p , q 3 p 3 n 3 + q ( 3 p 2 + 3 q p + q 3 ) [ n 1 ] p , q b n 2 x 2 [ n ] p , q 3 p 2 n 4 + q 3 ( 3 p 2 + 2 p q + q 2 ) [ n 1 ] p , q [ n 2 ] p , q b n x 3 [ n ] p , q 3 p n 3 + q 6 [ n 1 ] p , q [ n 2 ] p , q [ n 3 ] p , q x 4 [ n ] p , q 3 .
From Lemma 1, we have following:
Lemma 2.
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) 1 ; x , y = 1 , C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s ; x , y = x , C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) t ; x , y = y , C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s t ; x , y = x y , C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s 2 ; x , y = p 1 n 1 α n [ n ] p 1 , q 1 x + q 1 [ n 1 ] p 1 , q 1 [ n ] p 1 , q 1 x 2 , C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) t 2 ; x , y = p 2 m 1 β m [ m ] p 2 , q 2 y + q 2 [ m 1 ] p 2 , q 2 [ m ] p 2 , q 2 y 2 .
Using Lemma 2 and by linearity of C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) , we have
Remark 1.
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( t x ) 2 ; x , y = p 1 n 1 x 2 [ n ] p 1 , q 1 + x p 1 n 1 α n [ n ] p 1 , q 1 ,
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s y ) 2 ; x , y = p 2 m 1 y 2 [ m ] p 2 , q 2 + y p 2 m 1 β m [ m ] p 2 , q 2 .
Theorem 1.
Let q 1 : = ( q 1 , n ) , p 1 : = ( p 1 , n ) , q 2 : = ( q 2 , m ) , p 2 : = ( p 2 , m )
such that 0 < q 1 , n , q 2 , m < p 1 , n , p 2 , m 1 . If
lim n p 1 , n = 1 , lim n q 1 , n = 1 , lim m p 2 , m = 1 , lim m q 2 , m = 1 , lim n p 1 , n n = a 1 and lim m p 1 , m m = a 2 ,
the sequence C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ; x , y convergence uniformly to f ( x , y ) , on [ 0 , a ] × [ 0 , b ] = I a b for each f C I a b , where a , b be real numbers such that a α n , b β m and C ( I a b ) be the space of all real valued continuous function on I a b with the norm
f C ( I a b ) = sup ( x , y ) I a b f ( x , y ) .
Proof. 
Assume that the equities (7), (3) and (4) are holds. Then, we have
p 1 , n n 1 α n n p 1 , n , q 1 , n 0 , p 2 , m m 1 β m m p 2 , m , q 2 , m 0 , q 1 , n n p 1 , n , q 1 , n n p 1 , n , q 1 , n 1 and q 2 , m m 1 p 2 , m , q 2 , m m p 2 , m , q 2 , m 1 .
as n , m . From Lemma 2, we obtain lim n , m C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) e i j ; x , y = e i j ( x , y ) uniformly on I a b , where e i j ( x , y ) = x i y j , 0 i + j 2 are the test functions. By Korovkin’s theorem for functions of two variables was presented by Volkov [29], it follows that lim n , m C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ; x , y = f ( x , y ) , uniformly on I a b , for each f C ( I a b ) . □

3. Rate of Convergence

In this section, we analyze the convergence rates of the operators C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) to the function f ( x , y ) using the modulus of continuity. Furthermore, we will present a summary of the relevant notations and definitions concerning the modulus of continuity and Peetre’s K-functional for bivariate real-valued functions.
For a function f C ( I a b ) , the complete modulus of continuity in the bivariate context is defined as follows:
ω ( f , δ ) = sup | f ( t , s ) f ( x , y ) | : ( t x ) 2 + ( s y ) 2 δ .
for every ( t , s ) , ( x , y ) I a b . Additionally, the partial moduli of continuity concerning x and y are defined as follows:
ω 1 ( f , δ ) = sup | f ( x 1 , y ) f ( x 2 , y ) | : y [ 0 , b ] and | x 1 x 2 | δ ω 2 ( f , δ ) = sup | f ( x , y 1 ) f ( x , y 2 ) | : x [ 0 , a ] and | y 1 y 2 | δ ,
It is evident that they fulfill the properties of the standard modulus of continuity [11].
For δ > 0 , the Peetre-K functional [22] is defined as follows:
K ( f , δ ) = inf g C 2 ( I a b ) f g C ( I a b ) + δ g C 2 ( I a b ) ,
where C 2 ( I a b ) is the space of functions of f such that f, j f x j and j f y j ( j = 1 , 2 ) in C ( I a b ) . The norm . on the space C 2 ( I a b ) is defined by
f C 2 I a b = f C ( I a b ) + j = 1 2 j f y j C ( I a b ) + j f y j C ( I a b ) .
We now provide an estimate for the rate of convergence of the operators C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) .
Theorem 2.
Let f C I a b . For all x I a b , we have
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) | 2 ω f ; δ n , m ,
where
δ n , m 2 = a α n p 1 n 1 [ n ] p 1 , q 1 + b β m p 2 m 1 [ m ] p 2 , q 2 .
Proof. 
By definition, the complete modulus of continuity of f ( x , y ) , along with the linearity and positivity of our operator, allows us to express:
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) | C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | f ( t , s ) f ( x , y ) | C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ω f ; ( t x ) 2 + ( s y ) 2 ω ( f , δ n , m ) 1 δ n , m C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( t x ) 2 + ( s y ) 2 .
Using Cauchy-Scwartz inequality, from (5) and (6), one can write following
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) | ω ( f , δ n , m ) 1 + 1 δ n , m C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( t x ) 2 + ( s y ) 2 1 / 2 = ω ( f , δ n , m ) 1 + 1 δ n , m C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( t x ) 2 + C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s y ) 2 1 / 2 ω ( f , δ n , m ) 1 + 1 δ n , m a α n p 1 n 1 [ n ] p 1 , q 1 + b β m p 2 m 1 [ m ] p 2 , q 2 1 / 2 .
Choosing δ n , m = a α n p 1 n 1 [ n ] p 1 , q 1 + b β m p 2 m 1 [ m ] p 2 , q 2 1 / 2 , for all ( x , y ) I a b , we get desired the result.
Theorem 3.
Let f C I a b , then the following inequalities satisfy
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) | ω 1 f ; δ n + ω 2 f ; δ m ,
where
δ n 2 = a α n p 1 n 1 [ n ] p 1 , q 1 ,
δ m 2 = b β m p 2 m 1 [ m ] p 2 , q 2 .
Proof. 
By definition, the partial moduli of continuity of f ( x , y ) and the application of the Cauchy-Schwarz inequality imply that:
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) | C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | f ( t , s ) f ( x , s ) + f ( x , s ) f ( x , y ) | C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | f ( t , s ) f ( x , s ) | + C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | f ( x , s ) f ( x , y ) | C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | ω 1 ( f ; | t x | ) | + C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | ω 2 ( f ; | s y | ) | ω 1 ( f , δ n ) 1 + 1 δ n C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | t x | + ω 2 ( f , δ m ) 1 + 1 δ m C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | s y | ω 1 ( f , δ n ) 1 + 1 δ n C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( t x ) 2 1 / 2 + ω 2 ( f , δ m ) 1 + 1 δ m C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s y ) 2 1 / 2 .
Consider (5), (6) and choosing
δ n 2 = a α n p 1 n 1 [ n ] p 1 , q 1 , δ m 2 = b β m p 2 m 1 [ m ] p 2 , q 2 .
we reach the result. □
For α ^ 1 , α ^ 2 ( 0 , 1 ] and ( s , t ) , ( x , y ) I a b , we define the Lipschitz class L i p M ( α ^ 1 , α ^ 2 ) for the bivariate case as follows:
f ( t , s ) f ( x , y ) M t x α ^ 1 s y α ^ 2 .
Theorem 4.
Let f L i p M ( α ^ 1 , α ^ 2 ) . Then, for all ( x , y ) I a b , we have
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) | M δ n α ^ 1 / 2 δ m α ^ 2 / 2 ,
where δ n and δ m defined in (8) and (9), respectively.
Proof. 
As f L i p M ( α ^ 1 , α ^ 2 ) , it follows
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) | C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( | f ( t , s ) f ( x , y ) | ; x , y ) M C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( | t x | α ^ 1 | s y | α ^ 2 ; x , y ) = M C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( | t x | α ^ 1 | ; x ) C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( | s y | α ^ 2 ; y ) .
For p ^ = 1 α ^ 1 , q ^ = α ^ 1 2 α ^ 1 and p ^ = 1 α ^ 2 , q ^ = α ^ 2 2 α ^ 2 applying the Hölder’s inequality, we get
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) | M { C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( | t x | 2 ; x ) } α ^ 1 / 2 { C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( 1 ; x ) } α ^ 1 / 2 × { C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( | s y | 2 ; y ) } α ^ 12 / 2 { C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( 1 ; y ) } α ^ 2 / 2 = M δ n α ^ 1 / 2 δ m α ^ 2 / 2 .
Hence, we obtain the desired result. □
Theorem 5.
Let f C 1 ( I a b ) and 0 < q 1 , n , q 2 , m < p 1 , n , p 2 , m 1 . Then, we have
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t ) f ( s ) | f x C ( I a b ) δ n + f y C ( I a b ) δ m .
Proof. 
For ( t , s ) I a b , we obtain
f ( t ) f ( s ) = x t f u ( u , s ) d u + y s f v ( x , v ) d v
By applying our operator to both sides of the above equation, we deduce:
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t ) f ( s ) | C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) x t f u ( u , s ) d u ; x , y + C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) y s f v ( x , v ) d v ; x , y .
As
x t f u ( u , s ) d u f x C ( I a b ) | t x | and y s f v ( x , v ) d v f y C ( I a b ) | s y | ,
we have
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t ) f ( s ) | f x C ( I a b ) C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | t x | ; x , y + f y C ( I a b ) C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) | s y | ; x , y .
Using the Cauchy-Schwarz inequality, we can write following
| C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t ) f ( s ) | f x C ( I a b ) { C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( t x ) 2 ; x , y } 1 / 2 { C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) 1 ; x , y } 1 / 2 + f y C ( I a b ) { C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s y ) 2 ; x , y } 1 / 2 { C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) 1 ; x , y } 1 / 2 .
Form (5) and (6), we get desired the result. □
Below, we obtained three-dimensional graphs illustrating the convergence rates of operators to specific functions using the Maple [30] software.
Example 1. Figure 1 shows the optimal approximation of operators
C 20 , 20 ( 0.999 , 0.9 ) , ( 0.999 , 0.9 ) ( f ; x , y ) (red), C 20 , 20 ( 0.90 , 0.86 ) , ( 0.996 , 0.89 ) ( f ; x , y ) (yellow)
with α n = ln ( n ) , β m = m to function f ( x , y ) = 3 x y 2 e y (blue).
Figure 1. Convergence of two-dimensional ( p , q ) Bernstein-Chlodowsky polynomials.
Figure 1. Convergence of two-dimensional ( p , q ) Bernstein-Chlodowsky polynomials.
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Example 2. Figure 2 shows the optimal approximation of operators C 20 , 20 ( 0.999 , 0.9 ) , ( 0.99 , 0.9 ) ( f ; x , y ) (red), C 20 , 20 ( 0.990 , 0.86 ) , ( 0.996 , 0.89 ) ( f ; x , y ) (yellow)
with α n = ln ( n ) , β m = m to function f ( x , y ) = sin ( x y ) (blue).
Figure 2. Convergence of two-dimensional ( p , q ) Bernstein-Chlodowsky polynomials.
Figure 2. Convergence of two-dimensional ( p , q ) Bernstein-Chlodowsky polynomials.
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Example 3. Figure 3 shows the optimal approximation of operators
C 20 , 20 ( 0.99 , 0.9 ) , ( 0.999 , 0.96 ) ( f ; x , y ) (red), C 20 , 20 ( 0.99 , 0.9 ) , ( 0.990 , 0.90 ) ( f ; x , y ) (yellow)
with α n = ln ( n ) , β m = ln ( m ) to function f ( x , y ) = x 2 y x y 2 ) (blue).
Figure 3. Convergence of two-dimensional ( p , q ) Bernstein-Chlodowsky polynomials.
Figure 3. Convergence of two-dimensional ( p , q ) Bernstein-Chlodowsky polynomials.
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Theorem 6.
Let f C I a b , then we have
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ; x , y f ( x , y ) C I a b 2 M f ; δ n , m ( x , y ) / 2 ,
where
δ n , m ( x , y ) = 1 2 max a α n p 1 n 1 [ n ] p 1 , q 1 , b β m p 2 m 1 [ m ] p 2 , q 2 .
Proof. 
Let g C 2 ( I a b ) . Utilizing Taylor’s formula, we derive:
g ( s 1 , s 2 ) g ( x , y ) = g ( s 1 , y ) g ( x , y ) + g ( s 1 , s 2 ) g ( s 1 , y ) = g ( x , y ) x ( s 1 x ) + x s 1 ( s 1 u ) 2 g ( u , y ) u 2 d u + g ( x , y ) x ( s 2 y ) + y s 2 ( s 2 v ) 2 g ( x , v ) v 2 d v = g ( x , y ) x ( s 1 x ) + 0 s 1 x ( s 1 x u ) 2 g ( u , y ) u 2 d u + g ( x , y ) x ( s 2 y ) + 0 s 2 y ( s 2 y v ) 2 g ( x , v ) v 2 d v
By applying C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) to both sides of the above equation, we obtain:
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) g ( s 1 , s 2 ) g ( x , y ) g ( x , y ) x C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s 1 x ) ; x , y + C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) 0 s 1 x ( s 1 x u ) 2 g ( u , y ) u 2 d u ; x , y + g ( x , y ) y C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s 2 y ) ; x , y + C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) 0 s 2 y ( s 2 y v ) 2 g ( v , x ) v 2 d v ; x , y
As C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s 1 x ) ; x , y = 0 and C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s 2 y ) ; x , y = 0 , one can write following
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) g ( s 1 , s 2 ) g ( x , y ) C I a b 1 2 g ( x , y ) x C I a b C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s 1 x ) 2 ; x , y + 1 2 g ( x , y ) y C I a b C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s 2 y ) 2 ; x , y .
By (5), (6), we deduce,
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) g ( s 1 , s 2 ) g ( x , y ) C I a b 1 2 max p 1 n 1 x 2 [ n ] p 1 , q 1 + x p 1 n 1 α n [ n ] p 1 , q 1 , p 2 m 1 y 2 [ m ] p 2 , q 2 + y p 2 m 1 β m [ m ] p 2 , q 2 × g ( x , y ) x C I a b + g ( x , y ) x C I a b g C I a b δ n , m .
By the linearity C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) , we obtain
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ; x , y f ( x , y ) C I a b C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) g C I a b + C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) g g C I a b + f g C I a b .
By (10) and (11), one can see that
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ; x , y f ( x , y ) C I a b 2 M f ; δ n , m ( x , y ) / 2 .
This step completes the proof. □
Initially, we need to establish the auxiliary result found in the subsequent lemma.
Lemma 3.
Let 0 < q n < p n 1 be sequences such that p n , q n 1 and p n n a 1 as n . Then, we have the following limits:
(i) 
lim n [ n ] p n , q n α n C n , n ( p n , q n ) ( ( t x ) 2 ; x ) = a 1 x
(ii) 
lim n [ n ] p n , q n 2 α n 2 C n , n ( p n , q n ) ( ( t x ) 4 ; x ) = 3 a 1 x 2 .
Proof. (i) Using Lemma 1, we have
C n , n ( p n , q n ) ( ( t x ) 2 ; x ) = p n n 1 x 2 [ n ] p n , q n + x p n n 1 α n [ n ] p n , q n
Then, we get
[ n ] p n , q n α n C n , n ( p n , q n ) ( ( t x ) 2 ; x ) = p n n 1 x 2 α n + x p n n 1 .
Taking the limit of both sides of the above equality as n , we can write:
lim n [ n ] p n , q n α n C n , n ( p n , q n ) ( ( t x ) 2 , x ) = lim n p n n 1 x 2 α n + x p n n 1 = a 1 x .
(ii) Utilizing Lemma 1 along with the linearity of the operators C n , n ( p n , q n ) , we arrive at:
C n , n ( p n , q n ) ( ( t x ) 4 ; x ) = A 1 , n x 4 + A 2 , n x 3 + A 3 , n x 2 + A 4 , n x
where
A 1 , n = p n n 3 [ n ] p n , q n 2 ( p n 2 + 2 p n q n q n 2 ) + p n n 5 [ n ] p n , q n ( p n 3 + 3 p n q n 2 + q n 3 ) p n 3 n 6 ( p n 2 + p n 3 + 2 p n q n 2 + q n 3 ) [ n ] p n , q n 3 A 2 , n = p n n 3 [ n ] p n , q n 2 ( p n 2 2 p n q n + q n 2 ) [ n ] p n , q n 3 α n + p 2 n 5 [ n ] p n , q n ( q n 3 4 p n q n 2 3 p n 2 q n + 2 p n 3 ) p n 3 n 6 ( 3 p n 3 + 3 p n q n 2 + 5 p n 2 q n + q n 3 ) [ n ] p n , q n 3 α n A 3 , n = p n 2 n 4 [ n ] p n , q n ( p n 2 + 3 p n q n + q n 2 ) p n 3 n 5 ( 3 p n 2 + q n 2 + 3 p n q n ) [ n ] p n , q n 3 α n 2 A 4 , n = p 3 n 3 α n 3 [ n ] p n , q n 3 ,
It is clear that
lim n [ n ] p n , q n 2 α n 2 { A 4 , n x } = 0 .
Taking the limit of both sides of A 1 , n , we arrive at:
lim n [ n ] p n , q n 2 α n 2 { A 1 , n } = lim n p n n 3 [ n ] p n , q n ( p n q n ) 2 α n 2 + p n n 5 ( p n 3 + 3 p n q n 2 + q n 3 ) α n 2 p n 3 n 6 ( p n 2 + p n 3 + 2 p n q n 2 + q n 3 ) [ n ] p n , q n α n 2 = lim n p n n 3 ( p n n q n n ) ( p n q n ) α n 2 + p n 5 ( p n 3 + 3 p n q n 2 + q n 3 ) α n 2 p n 3 n 6 ( p n 2 + p n 3 + 2 p n q n 2 + q n 3 ) [ n ] p n , q n α n 2 = 0 .
Similarly, we can show that;
lim n [ n ] p n , q n 2 α n 2 { A 2 , n } = 0 and lim n [ n ] p n , q n 2 α n 2 { A 3 , n } = 3 a 1 x 2
By combining (14)-(16), we reach the desired the result. □
Now, we ready present a Voronovskaja type theorem for C n , n ( p n , q n ) ( f ; x , y ) .
Theorem 7.
Let f C 2 ( I a b ) . Then, we have
lim n [ n ] p n , q n C n , n ( p n , q n ) ( f ; x , y ) f ( x , y ) ) = a 1 x f x 2 ( x , y ) 2 + a 1 y f y 2 ( x , y ) 2 .
Proof. 
Let ( x , y ) I a b . Then, write Taylor’s formula of f as follows:
f ( s , t ) = f ( x , y ) + f x ( s x ) + f y ( t y ) + 1 2 f x 2 ( t x ) 2 + 2 f x y ( s x ) ( t y ) + f y 2 ( t y ) 2 + ε ( s , t ) ( s x ) 2 + ( t y ) 2
where ( s , t ) I a b and ε ( s , t ) 0 as ( s , t ) ( x , y ) .
If we apply the operator C n , n ( p n , q n ) ( f ; s , t ) on (17), we obtain
C n , n ( p n , q n ) ( f ; s , t ) f ( x , y ) = f x ( x , y ) C n , n ( p n , q n ) ( ( s x ) ; x , y ) + f y ( x , y ) C n , n ( p n , q n ) ( ( t y ) ; x , y ) + 1 2 { f x 2 C n , n ( p n , q n ) ( ( t x ) 2 ; x , y ) + 2 f x y C n , n ( p n , q n ) ( ( s x ) ( t y ) ; x , y ) + f y 2 C n , n ( p n , q n ) ( ( t y ) 2 ; x , y ) } + C n , n ( p n , q n ) ε ( s , t ) ( s x ) 2 + ( t y ) 2 ; x , y .
Applying the limit of both sides of the above equality, we get n , □
lim n [ n ] p n , q n C n , n ( p n , q n ) ( f ; s , t ) f ( x , y ) ) = lim n [ n ] p n , q n 1 2 { f x 2 C n , n ( p n , q n ) ( ( t x ) 2 ; x , y ) + 2 f x y C n , n ( p n , q n ) ( ( s x ) ( t y ) ; x , y ) + f y 2 C n , n ( p n , q n ) ( ( t y ) 2 ; x , y ) } + lim n [ n ] p n , q n C n , n ( p n , q n ) ε ( s , t ) ( s x ) 2 + ( t y ) 2 ; x , y .
By Cauchy-Schwartz inequality, we can write the following
C n , n ( p n , q n ) ε ( s , t ) ( s x ) 2 + ( t y ) 2 ; x , y lim n C n , n ( p n , q n ) ε 2 ( s , t ) ; x , y × 2 lim n [ n ] p n , q n 2 C n , n ( p n , q n ) ε ( s , t ) ( s x ) 4 + ( t y ) 4 ; x , y .
As lim n C n , n ( p n , q n ) ε 2 ( s , t ) ; x , y = ε 2 ( x , y ) = 0 and from Lemma 3(ii)
lim n [ n ] p n , q n 2 C n , n ( p n , q n ) ( s x ) 4 + ( t y ) 4 ) ; x , y is finite, then we have
lim n [ n ] p n , q n 2 C n , n ( p n , q n ) ε ( s , t ) ( s x ) 4 + ( t y ) 4 ; x , y = 0 .
Hence, we deduce
lim n [ n ] p n , q n C n , n ( p n , q n ) ( f ; x , y ) f ( x , y ) ) = a 1 x f x 2 ( x , y ) 2 + a 1 y f y 2 ( x , y ) 2 .
This step completes the proof.

4. Weighted Approximation Properties of Two Variable Function

In this section, we investigate the convergence of the sequence of linear positive operators C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) to a function of two variables defined within a weighted space. We also compute the rate of convergence using the weighted modulus of continuity.
Let ρ ( x , y ) = x 2 + y 2 + 1 , and define B ρ as the space of all functions f defined on the real axis that satisfy | f ( x , y ) | M f ρ ( x , y ) , where M f is a positive constant dependent solely on f. The subspace C ρ of B ρ consists of all continuous functions and is equipped with the norm:
f ρ = sup ( x , y ) R + 2 | f ( x , y ) | ρ ( x , y ) .
Let C ρ 0 represent the subspace of all functions f C ρ for which lim x f ( x , y ) ρ ( x , y ) exists and is finite. For every f C ρ 0 , the weighted modulus of continuity is defined as
Ω f ( f ; δ 1 , δ 2 ) = sup ( x , y ) R + 2 sup h 1 δ 1 , h 2 δ 2 f ( x + h 1 , y + h 2 ) f ( x , y ) ρ ( x , y ) ρ ( h 1 , h 2 ) .
Lemma 4.
The operators C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) defined (2) act from C ρ ( R + 2 ) to B ρ ( R + 2 ) if and only if the inequality
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( ρ ; x , y ) x 2 c .
holds for some positive constant c.
Theorem 8.
Consider the sequence of linear positive operators C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) defined in (2). For any function f C ρ 0 and for all points ( x , y ) I α n β m , it follows that
lim n C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( f ; x , y ) f ( x , y ) ρ = 0 .
Proof. 
From Lemma 2, we obtain
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) 1 ; x , y 1 ρ = 0 , C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s ; x , y x ρ = 0 C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) t ; x , y y ρ = 0 .
Again by Lemma 2, we can write following
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s 2 + t 2 ; x , y ) ( x 2 + y 2 ) ρ = sup ( x , y ) R + 2 p 1 n 1 α n x [ n ] p 1 , q 1 ( x 2 + y 2 + 1 ) + p 1 n 1 x 2 [ n ] p 1 , q 1 ( x 2 + y 2 + 1 ) + p 2 m 1 β m y [ m ] p 2 , q 2 ( x 2 + y 2 + 1 ) + p 2 m 1 y 2 [ m ] p 2 , q 2 ( x 2 + y 2 + 1 ) p 1 n 1 α n [ n ] p 1 , q 1 + p 1 n 1 [ n ] p 1 , q 1 + p 2 m 1 β m [ m ] p 2 , q 2 + p 2 m 1 [ m ] p 2 , q 2
Considering the limit of both sides of the preceding inequality as n , m and applying (3) and (4), we derive
lim m , n C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( s 2 + t 2 ; x , y ) ( x 2 + y 2 ) ρ = 0 .
Applying weighted Korovkin theorem for two variable which presented by Gadzhiev [4,5], we get desired the results. □
For estimate rate of convergence, we need the following lemma.
Lemma 5.
For all ( x ; y ) I α n β m , by (5), (6) and (13), one can write the following
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) t x 2 ; x , y = O α n p 1 n 1 [ n ] p 1 , q 1 x 2 + x ,
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) t x 4 ; x , y = O α n p 1 n 1 [ n ] p 1 , q 1 x 4 + x 3 + x 2 + x
and
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s y 2 ; x , y = O β m p 2 m 1 [ m ] p 2 , q 2 y 2 + y + 1 ,
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s y 4 ; x , y = O β m p 2 m 1 [ m ] p 2 , q 2 y 4 + y 3 + y 2 + y + 1 .
Now, compute rate of convergence the operator C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) in weighted spaces.
Theorem 9.
If f C ρ 0 , then we have
sup x , y R + 2 C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( f ; x , y ) f ( x , y ) ρ x , y 3 C 2 ω ρ ( f ; δ n , δ m )
, where C 2 is a constant independent of n , m and δ n = p 1 n 1 α n [ n ] p 1 , q 1 , δ n = p 2 m 1 β m [ m ] p 2 , q 2 .
Proof. 
Taking into account the following inequality given in [9], we deduce
f t , s f x , y 8 1 + x 2 + y 2 ω ρ ( f ; δ n , δ m )
× 1 + t x δ n 1 + s y δ m 1 + t x 2 1 + s y 2 .
Applying C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) both side above inequality and using Cauchy-Schwarz inequality, one can write following
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) 8 1 + x 2 + y 2 ω ρ ( f ; δ n , δ m )
× 1 + C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) t x 2 ; x , y + 1 δ n C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) t x 2 ; x , y
1 δ n C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) t x 2 ; x , y C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) t x 4 ; x , y
× 1 + C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s y 2 ; x , y , a + 1 δ m C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s y 2 ; x , y
× 1 δ m C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s y 2 ; x , y C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) s y 4 ; x , y .
By (19)-(22), we obtain
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) 8 1 + x 2 + y 2 ω ρ ( f ; δ n , δ m )
× 1 + O p 1 n 1 α n [ n ] p 1 , q 1 x 2 + x + 1 δ n O p 1 n 1 α n [ n ] p 1 , q 1 x 2 + x
+ 1 δ n O p 1 n 1 α n [ n ] p 1 , q 1 x 2 + x x 4 + x 3 + x 2 + x
× 1 + p 2 m 1 β m [ m ] p 2 , q 2 y 2 + y + p 2 m 1 β m [ m ] p 2 , q 2 p 2 m 1 β m [ m ] p 2 , q 2
+ 1 δ m p 2 m 1 β m [ m ] p 2 , q 2 y 2 + y p 2 m 1 β m [ m ] p 2 , q 2 y 4 + y 3 + y 2 + y .
Taking δ n = p 1 n 1 α n [ n ] p 1 , q 1 1 / 2 , δ m = p 2 m 1 β m [ m ] p 2 , q 2 1 / 2 , one write the following:
C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) f ( t , s ) f ( x , y ) C 2 1 + x 2 + y 2 ω ρ ( f ; δ n , δ m )
× 1 + δ n 2 x 2 + x + x 2 + x + x 2 + x x 4 + x 3 + x 2 + x
× 1 + δ m 2 y 2 + y + y 2 + y + y 2 + y y 4 + y 3 + y 2 + y ,
where C 2 is a constant independent of n , m . Since δ n 2 < 1 , δ m 2 < 1 , for sufficiently large n , m , we get
sup x , y R + 2 C n , m ( p 1 , q 1 ) , ( p 2 , q 2 ) ( f ; x , y ) f ( x , y ) 1 + x 2 + y 2 3 C 2 ω ρ f ; p 1 n 1 α n [ n ] p 1 , q 1 , p 2 m 1 β m [ m ] p 2 , q 2 .
This step completes the proof. □

Author Contributions

Ü.K. was responsible for conceptualization; A.K. conducted the validation and formal analysis; A.A. handled the writing. All authors have reviewed and approved the manuscript’s final version.

Funding

This study did not receive any external funding.

Data Availability Statement

The data are available within the article itself.

Acknowledgments

We appreciate the referees for their meticulous examination of the original manuscript and for their constructive suggestions.

Conflicts of Interest

The authors state that there are no conflicts of interest to disclose.

Abbreviations

The following abbreviations are used in this manuscript:
MDPI Multidisciplinary Digital Publishing Institute
DOAJ Directory of open access journals
TLA Three letter acronym
LD Linear dichroism

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