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Approximation properties by shifted knots type of α-Bernstein–Kantorovich–Stancu operators
Journal of Inequalities and Applications volume 2024, Article number: 85 (2024)
Abstract
Through the real polynomials of the shifted knots, the α-Bernstein–Kantorovich operators are studied in their Stancu form, and the approximation properties are obtained. We obtain some direct approximation theorem in terms of Lipschitz type maximum function and Peetre’s K-functional, as well as Korovkin’s theorem. Eventually, the modulus of continuity is used to compute the upper bound error estimation.
1 Introduction and preliminaries
In 1912, it was established that for all continuous function g on the interval \([0,1]\) the classical Bernstein polynomials \(B_{s}(g;z)\) converge uniformly to g (see [9]). In 1968, for the real parameters α, β such that \(0\leq \alpha \leq \beta \), Stancu introduced another variant of Bernstein polynomial known as Bernstein–Stancu operators \(B_{s,\alpha ,\beta}(g;z)\) such that (see [28])
where \(z\in [0,1]\), \(z\in \mathbb{N}\), and Stancu in his investigation showed that \(B_{s,\alpha ,\beta}\) is uniformly convergent to the continuous function g in \([0,1]\).
In the year 2017, Chen et al. [12] proposed the generalization of Bernstein operators with shape parameter \(\alpha \in [0,1]\). These operators are defined as follows:
where \(g\in C[0,1]\) and \(g_{i}=g\left ( \frac{i}{s}\right )\). For \(s>2\), the polynomial \(\tilde{b}_{s,i}(\alpha ;z)\) of degree s is defined by \(\tilde{b}_{1,0}(\alpha ;z)=1-z\), \(\tilde{b}_{1,1}(\alpha ;z)=z\), and
and the binomial coefficient \(\binom{s}{i}\) is given by
Mohiuddine et al. [19] provided the Kantorovich variant of operators (2). Numerous authors have repeatedly presented various generalizations of the aforementioned operators and established approximation results. For instance, Schurer modification of operators (2) was covered in Özger et al. [23].
In a more recent work, the Bernstein–Stancu polynomials are presented using shifted knots with new parameters in the following way (see [13]):
where \(z\in [\frac{\alpha _{2}}{s+\beta _{2}}, \frac{s+\alpha _{2}}{s+\beta _{2}}]\) and \(\alpha _{i}\), \(\beta _{i}\), \(i=1,2\), are positive real numbers provided \(0\leq \alpha _{2} \leq \alpha _{1} \leq \beta _{1} \leq \beta _{2}\). Researchers in approximation processes have recently developed Bernstein type operators; for example, we choose [1, 21, 29]. The relevant results for this article have been studied in various functional spaces such as Phillips operators via q-Dunkl generalization [2], Approximation by α-Baskakov-Jain type operators [15], Durrmeyer-type generalization of μ-Bernstein operators [16], modified λ-Bernstein polynomial [7], Kantorovich q-Baskakov operators [6], Szász–Durrmeyer operators [5], Bézier bases with Schurer polynomials [22], Stancu-type λ-Schurer [4], λ-Bernstein operators [10, 11], q- Szász–Durrmeyer type operators [26], Stancu variant of generalized Baskakov operators [25], and modified Baskakov–Durrmeyer operators [24].
In this work, we highlight the following main notion. The fundamental definitions and characteristics of Bernstein operators are covered in the first part. In the second part, we employ the shifted knot parameters to construct a new family of generalized α-Bernstein operators, including the Stancu–Kantorovich variation. We demonstrate that these new operators are essential to the theory of uniform approximation. In the third, fourth, and fifth sections, we examine the new operators’ shape-preserving features, rate of convergence, and several direct theorems.
Recently, the authors have developed the Stancu variation of Bernstein–Kantorovich operators based on the shape parameter α (fixed real) by [20] for the set of all continuous functions defined on \([0,1]\).
where
and the parameters satisfy the condition \(0\leq s_{1}\leq t_{1}\).
2 Construction of operators
We offer an extension of Stancu type α-Bernstein–Kantorovich operators in this section, exploring some approximation results through the use of shifted knots. Let \(1\leq p<\infty \), \(\mathcal{I}_{s}=[\frac{\zeta _{2}}{\varkappa _{2}+1+s}, \frac{\zeta _{2}+1+s}{\varkappa _{2}+1+s}]\) and \(s\geq 2\), \(s\in \mathbb{N}\). Given \(\mathcal{J}_{s,\alpha}^{\ast }: L_{p}[0,1]\rightarrow L_{p}( \mathcal{I}_{s})\), we define shifted knots of α-Bernstein–Kantorovich–Stancu type polynomials (5) as follows: For every \(g \in L_{p}[0,1]\) and any fixed real α, we write
where \(\frac{\zeta _{2}}{\varkappa _{2}+1+s}\leq z \leq \frac{\zeta _{2}+1+s}{\varkappa _{2}+1+s}\), \(\zeta _{i}\), \(\varkappa _{i} \) (\(i=1,2\)) are positive real numbers, indeed \(0\leq \zeta _{2} \leq \zeta _{1} \leq \varkappa _{1} \leq \varkappa _{2} \). It is very clear to note that if \(\zeta _{2} =\varkappa _{2}=0\) then the α-Bernstein–Stancu variant of Kantorovich polynomial is given in [20]. And in case of \(\zeta _{1}=\zeta _{2} =\varkappa _{1}=\varkappa _{2}=0\) the classic α-Bernstein–Kantorovich polynomial is obtained in [19] and \(\mathcal{Q}_{s,\alpha}^{\ast }(z)\) is given as follows:
Our motive to construct the Stancu type α-Bernstein–Kantorovich shifted knot operators gives a valuable research path to a researcher in the field of approximation theory. The researcher can use the shifted knot operators with a shape parameter \(\alpha \in [0,1]\) in various Bernstein type operators and can explore them to get a better observation and more flexibility. For example, in our future work we commit to apply these operators to the Bernstein operators by Bézier bases function. For more related results and applications of Bernstein type and shifted knot type operators, we refer to [10, 11, 13, 29]. Moreover, the Bernstein and Bernstein–Stancu polynomials are used in many branches of mathematics and computer science (see [8, 18]).
The primary goal of this paper is to use the integral modulus of continuity and the modulus of continuity to study the approximation properties of operators (6). Ultimately, we derive the convergence of operators (6) using Peetre’s K-functional and Lipschitz maximal functions. Let us do some simple manipulation here, so we take
If it corresponds to term \(i=s\) in \(J_{1}\) and \(i=0\) in \(J_{2}\), then \(\binom{s-2}{s}=0\) and \(\binom{s-2}{-2}=0\). Thus
Clearly, replace i by \(i+1\) in \(J_{2}\), then
Therefore, it follows that
where \(\binom{s-2}{i}=\left ( 1- \frac{i}{s-1}\right )\binom{s-1}{i}\) and \(\binom{s-2}{i-1}=\frac{i}{s-1}\binom{s-1}{i}\). Hence we have
where
In addition, we take any function \(g \in L_{p}[0,1]\), then for all \(z\in \mathcal{I}_{s} \), \(s\geq 2\), \(s\in \mathbb{N}\) operators (6) are also calculated as
where \(f_{i}\) is defined by (8), α is any fixed real and
Lemma 1
Suppose that the test function \(\chi _{j}(t)=t^{\mu }\) for \(\mu =0,1,2\), then for all \(z \in \mathcal{I}_{s}\) operators (6) have the following identities:
Proof
If \(\mu =0\), \(\chi _{0}(t)=1\), then we are able to see that from (9)
For \(\mu =1\), \(\chi _{1}(t)=t\), we get
From a simple calculation we see that
Therefore, we get
For \(\mu =2\), \(\chi _{2}(t)=t^{2}\), we obtain
Therefore,
This completes the proof of Lemma 1. □
Lemma 2
Operators \(\mathcal{M}_{s,\alpha}^{\ast }(. \,;\, .)\) have the central moments as follows:
where \(\mathcal{M}_{s,\alpha}^{\ast }(\chi _{j}(t);z) \) for all \(j=0,1,2\) are defined by Lemma 1.
Theorem 1
Let \(z \in \mathcal{I}_{s}\), then for the continuous function g on \([0,1]\), it follows that
Proof
Taking into account the equality in Lemma 1, it is easy to write
We are denoting
It is easy to get
On the other hand, from (11) and (13) we obviously get
Applying the well-known Korovkin’s theorem [17] to the sequence of operators \(\mathcal{R}_{s,\alpha}^{\ast}\), from this fact it is easy to see for all \(g\in C[0,1] \) on \([0,1]\)
Thus, (13) gives us
where \(C[0,1]\) is the set of all continuous function g on \([0,1]\). This completes the proof. □
Theorem 2
Let \(g\in L_{p}[0,1]\), \(p \in [1,\infty )\), then operators (6) satisfy
Proof
Theorem 1 is taken into consideration for the proof along with the operators \(\mathcal{R}_{s,\alpha}^{\ast}\) by (12). According to the Luzin theorem, there is a continuous function ϕ on \([0,1]\) such that \(\|g-\phi \|_{L_{p}[0,1]}<\epsilon \) for given \(\epsilon >0\). Let \(L_{p}[0,1]\rightarrow L_{p}[0,1]\) be the operator with (12) and \(\|\mathcal{R}_{s,\alpha}^{\ast}\|\) be the operator norm. Then, for any \(s\in \mathbb{N}\), it is sufficient to demonstrate that there exists a positive number M such that \(\|\mathcal{R}_{s,\alpha}^{\ast}\|\leq M\) to support the conclusions made by Theorem 2. We employ Theorem 1 for this purpose, which states that for any \(\epsilon >0\), there exists a number \(s_{0}\in \mathbb{N}\), \(s\geq s_{0}\) such that \(\|\mathcal{R}_{s,\alpha}^{\ast}(\phi ;z)-\phi (z)\|_{C[0,1]}< \epsilon \).
From these facts, we immediately consider
To get positive S, we apply Jensen’s inequality to operators (6)
Therefore,
In the next, from operators (12), we have the inequality \(\int _{[0,1]\setminus \mathcal{I}_{s}}|g(z)|^{p}\mathrm{d}z \leq \|g\|_{L_{p}[0,1]}^{p} \). Thus we find that
Therefore we can write expression (15)
From the above fact it follows that, for all \(s\in \mathbb{N}\), there exists a positive M such that \(\|\mathcal{R}_{s,\alpha}^{\ast}\|\leq M\). Therefore, from (14) we deduce that
Similarly, taking into account the above inequality, we also see
These explanations give us \(\lim _{s \to \infty} \|\mathcal{M}_{s,\alpha}^{\ast}(g;z)-g(z)\|_{L_{p}( \mathcal{I}_{s})} =0\), this completes the proof of Theorem 2. □
3 Rate of convergence of \(\mathcal{M}_{s,\alpha}^{\ast }\)
Finding the degree of approximation for a series of operators \(\mathcal{M}_{s,\alpha}^{\ast }\) is our goal in this section. Recalling the modulus of continuity of function g (see [3]), we employ \(g\in C[0,1]\), the set of all continuous functions on \([0,1]\), and a positive value \(\delta ^{\ast}\), thus
As a result, we express the general estimate theorem developed by Shisha and Mond (see [27]) in terms of the modulus of continuity as follows to ascertain the order of convergence.
Theorem 3
[27] Let \([c,d]\subset [a,b]\) and \(\{L_{s}\}_{s \geq 1}\) be the sequence of positive linear operators from \(C[a,b]\) to \(C[c,d]\).
-
(1)
If \(g\in C[a,b]\) and \(z \in [c,d]\), then we have
$$\begin{aligned} |L_{s}(g;z)-g(z)| \leq & |g(z)| |L_{s}(\chi _{0}(t);z)-1| \\ +& \big\{ L_{s}(\chi _{0}(t);z)+ \frac{1}{\delta ^{\ast}} \sqrt{L_{s}((t-z)^{2};z)} \sqrt{L_{s}(\chi _{0}(t);z)} \big\} \omega ^{\ast}(g;\delta ^{\ast}). \end{aligned}$$ -
(2)
If \(g^{\prime }\in C[a,b]\) and \(z \in [c,d]\), then we have
$$\begin{aligned} |L_{s}(g;z)-g(z)| \leq & |g(z)| |L_{s}(\chi _{0}(t);z)-1| + |g^{ \prime }(z)| |L_{s}(t-z;z)| \\ + &L_{s}((t-z)^{2};z) \big\{ \sqrt{L_{s}(\chi _{0}(t);z)} + \frac{1}{\delta ^{\ast}} \sqrt{L_{s}((t-z)^{2};z)}\big\} \omega ^{ \ast}(g^{\prime };\delta ^{\ast}). \end{aligned}$$
Theorem 4
Let the function g be continuous on \([0,1]\), then for each \(z \in \mathcal{I}_{s} \) operators (6) satisfy the inequality
where \(\delta _{s,\alpha}^{\ast}(z)= \frac{1}{\left (\frac{\varkappa _{2}+1+s}{s+1}\right )^{2} (1-\alpha )+\alpha \left (\frac{\varkappa _{2}+1+s}{s+1}\right )} \mathcal{M}_{s,\alpha}^{\ast }((\chi _{1}(t)-z)^{2};z)\).
Proof
If we utilize Lemma 2 and take into account (1) of Theorem 3, we can write
If we choose \(\delta ^{\ast}=\sqrt{\delta _{s,\alpha}^{\ast}(z)}= \frac{1}{\sqrt{\left (\frac{\varkappa _{2}+1+s}{s+1}\right )^{2} (1-\alpha )+\alpha \left (\frac{\varkappa _{2}+1+s}{s+1}\right )} } \sqrt{\mathcal{M}_{s,\alpha}^{\ast }((\chi _{1}(t)-z)^{2};z)}\), then we get the desired result. □
Theorem 5
Let \(z\in \mathcal{I}_{s}\), then for every \(g\in C[0,1]\), it follows that
where \(\tilde{\delta}=\max _{z \in \mathcal{I}_{s} }\delta _{s,\alpha}^{ \ast}(z)\).
Proof
We easily obtain the desired result due to the monotonicity of the modulus of continuity. □
Remark 1
The order of the local approximation is estimated by Theorem 4, and the global order is estimated by Theorem 5 when we examine the approximation for each point \(z \in \mathcal{I}_{s}\).
Theorem 6
Let \(g^{\prime}\in C[0,1]\), then for each \(z \in \mathcal{I}_{s} \) we have
where \(\mathcal{M}_{s,\alpha}^{\ast }(\chi _{0}(t);z)=\left ( \frac{\varkappa _{2}+1+s}{s+1}\right )^{2} (1-\alpha )+\alpha \left ( \frac{\varkappa _{2}+1+s}{s+1}\right )\) and \(\delta _{s,\alpha}^{\ast}(z)\) is defined in Theorem 4.
Proof
We consider (2) of Theorem 3 and Lemma 1; as a result, we can write quickly
which completes the proof asserted by Theorem 6. □
4 Some direct approximation theorem to \(\mathcal{M}_{s,\alpha}^{\ast }\)
Here, too, we examine the approximation in \(L_{p}\) spaces thanks to some preliminary data. The \(L_{p}\) spaces on \(\mathcal{I}_{s}\) are taken for this purpose for every \(p \in [1,\infty )\) as \(L_{p}(\mathcal{I}_{s})\). Lastly, we derive the corresponding estimate in the \(L_{p}(\mathcal{I}_{s})\) spaces. In fact, the integral modification in terms of modulus of continuity for every \(g\in L_{p}(\Theta _{\varkappa})\) is provided by
where \(\| .\| _{L_{p}(\Theta _{\varkappa})}\) denotes the \(L_{p}\) norm over \(\Theta _{\varkappa}=[0,1-\varkappa ]\). To measure the smoothness, we use Peetre’s K-functional, and for this purpose we take \(\mathcal{Z}_{1,p}(\Theta _{\varkappa})=\{ g, g^{\prime} \in L_{p}( \Theta _{\varkappa}): g \text{ is absolutely continuous} \}\). Let \(1\leq p <\infty \), then for any \(g\in L_{p}(\Theta _{\varkappa})\) Peetre’s K-functional is defined as follows:
Moreover, for the positive constants \(c_{1}\) and \(c_{2}\), the equivalence of relations between integral modulus of continuity and Peetre’s K-functional is given by the inequality (see [14])
Taking into account operators (6) and Lemma 1, let us denote \(\mathcal{M}_{i} =[\frac{i+\zeta _{1}}{\varkappa _{1}+1+s}, \frac{i+\zeta _{1}+1}{\varkappa _{1}+1+s}]\)
and
Theorem 7
Let \(g\in \mathcal{Z}_{1,p}[0,1]\), \(p>1\), then operators \(\mathcal{T}_{s,\alpha}^{\ast }\) by (20) satisfy the inequality
where \(\mathcal{T}_{s,\alpha}^{\ast }\left (\chi _{2}(t);z \right )\) is defined by (20).
Proof
For any fixed \(z\in \mathcal{I}_{s} \), we easily get that
where \(\Phi _{g^{\prime}}(z)=\sup _{t\in [0,1]}\frac{1}{t-z} \int _{z}^{t} \left \vert g^{\prime}(\lambda )\right \vert \mathrm{d}\lambda \) for \(t\neq z\) is the Hardy–Littlewood majorant of \(g^{\prime}\). Applying the well-known Cauchy–Schwarz inequality, we get
where from the Hardy–Littlewood theorem [30] we get
Thus, for any \(1< p<\infty \), we get that
□
Theorem 8
For any \(g\in L_{p}[0,1]\) with the number \(1< p<\infty \), operators (20) verify the inequality
where \(\mathcal{C}=2 c_{2}+2^{\frac{1}{p}}\left (\frac{p}{p-1} \right )\) is a positive constant and \(\zeta _{s,\alpha}(z)=\max _{z\in \mathcal{I}_{s}}\bigg( \mathcal{T}_{s,\alpha}^{\ast }\left (\chi _{2}(t);z \right ) \bigg)^{ \frac{1}{2}}\).
Proof
Let us denote
where \(\zeta _{s,\alpha}(z)=\max _{z\in \mathcal{I}_{s}}\bigg( \mathcal{T}_{s,\alpha}^{\ast }\left (\chi _{2}(t);z \right ) \bigg)^{ \frac{1}{2}}\).
For an arbitrary function \(g\in \mathcal{Z}_{1,p}[0,1]\), the positive linear operators imply that
□
Theorem 9
For an arbitrary function \(g\in C^{2}\lbrack 0,1 \rbrack \), let the auxiliary operators \(\mathcal{R}_{s,\alpha}^{\ast }\) be such that
Then, for every \(\phi \in C^{2}\lbrack 0,1 \rbrack \), it follows that
where \(\zeta _{s,\alpha}^{\ast}(z)= \frac{1}{\left (\frac{\varkappa _{2}+1+s}{s+1}\right )^{2} (1-\alpha )+\alpha \left (\frac{\varkappa _{2}+1+s}{s+1}\right )} \mathcal{T}_{s,\alpha}^{\ast }\left (\chi _{1}(t);z\right )\) and \(\mathcal{T}_{s,\alpha}^{\ast }\left (\chi _{1}(t);z\right )\) is defined by (20). In addition, \(C^{2}\lbrack 0,1 \rbrack \) is defined by
Proof
For any \(\phi \in C^{2}\lbrack 0,1 \rbrack \), we easily get \(\mathcal{R}_{s,\alpha}^{\ast }(\chi _{0}(t);z)=1\) and
From the Taylor series, we see
By use of the linearity of \(\mathcal{R}_{s,\alpha}^{\ast }\), we get
where \(\zeta _{s,\alpha}^{\ast}(z)= \frac{1}{\left (\frac{\varkappa _{2}+1+s}{s+1}\right )^{2} (1-\alpha )+\alpha \left (\frac{\varkappa _{2}+1+s}{s+1}\right )} \mathcal{T}_{s,\alpha}^{\ast }\left (\chi _{1}(t);z\right )\). Thus
Since we know
and
we get
This gives the complete proof of Theorem 9. □
5 Graphical analysis
In this section, we give a numerical example with illustrative graphics with the help of MATLAB.
Example 1
Let \(g(y)=(y-\frac{1}{3})(y-\frac{3}{5})\), \(\xi _{1}=4\), \(\xi _{2}=3\), \(\chi _{1}=1.5\), \(\chi _{2}=4\), and \(s\in \{20,30,110\}\). The convergence of the operator towards the function \(g(y)\) is shown in Fig. 1.
From this example, we observe that approximation of function by the operators becomes better when we take larger values of s.
6 Conclusions
It is very clear that for the choices of \(\zeta _{2} =\varkappa _{2}=0\), our new constructed operators reduced to α-Bernstein–Stancu variant of Kantorovich polynomial given by [20]. For the choices of \(\zeta _{1}=\zeta _{2} =\varkappa _{1}=\varkappa _{2}=0\), our new constructed operators reduced to the classical α-Bernstein–Kantorovich polynomial obtained in [19]. Therefore, based on our research, we can conclude that the shifted knot operators defined by equality (6), which we have named our new Bernstein–Kantorovich variation, are an improved version of the previous operators defined by [19, 20]. This article’s major goal is to examine how operators that shifted knots of α-Bernstein–Kantorovich operators (6) in \(L_{p}\) spaces converge on \([0, 1]\).
Data Availability
No datasets were generated or analysed during the current study.
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The authors extend their appreciation to the Deanship of Scientific Research at University of Tabuk for Funding this work through Research no. S-0157-1443.
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Nasiruzzaman, M., Dilshad, M., Albalawi, B.M.E. et al. Approximation properties by shifted knots type of α-Bernstein–Kantorovich–Stancu operators. J Inequal Appl 2024, 85 (2024). https://doi.org/10.1186/s13660-024-03164-8
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DOI: https://doi.org/10.1186/s13660-024-03164-8