The main purpose of this paper is to introduce some approximation properties of a Kantorovich kind q-Bernstein operators related to Bézier basis functions with shape parameter λ∈[−1,1]. Firstly, we compute some basic results such as moments and central moments, and derive the Korovkin type approximation theorem for these operators. Next, we estimate the order of convergence in terms of the usual modulus of continuity, for the functions belong to Lipschitz-type class and Peetre’s K-functional, respectively. Lastly, with the aid of Maple software, we present the comparison of the convergence of these newly defined operators to the certain function with some graphical illustrations and error estimation table.
q-calculusλ-Bernstein polynomialsorder of convergenceLipschitz-type functionPeetre’s K-functionalIntroduction
One of the uncomplicated and most elegant proof of the Weierstrass approximation theorem, the polynomials introduced by Bernstein [1], still guides many studies. Very recently, the quantum calculus shortly (q-calculus), which has numerous applications in various disciplines, has attracted the attention of many authors working on approximation theory. Firstly, Lupaş [2] investigated several approximation properties of the generalizations of q-Bernstein polynomials. Afterward, Phillips [3] obtained some convergence theorems and Voronovskaya type asymptotic formula for the most popular generalizations of the q-Bernstein polynomials. Based on the studies [2,3], many approximation properties of the well-known linear positive operators via q-calculus were investigated in details by several researchers. We refer readers for some notable results [4–13].
In 2007, a Kantorovich type Bernstein polynomials via q-calculus are constructed by Dalmanoğlu [14] as follows:
where Bm,q:C[0,1]→C[0,1] are defined for any m∈N and any function μ∈C[0,1].
She obtained several approximation properties of the constructed polynomials (1) and estimated the order of approximation in terms of the modulus of continuity. Now, before proceeding further, we recall several basic notations based on q-calculus see details in [15]. Let 0<q≤1, for all integer j > 0, the q-integer [j] q is defined by
[j]q:={1−qj1−q,q≠1j,q=1.
The q-factorial [j] q! and q-binomial [jl]q are defined respectively, as below:
[j]q!:={[j]q[j-1]q..[1]q,j=1,2,..1,j=0
and
jlq:=[j]q![l]q![j-l]q!,(j≥l≥0).
The q-analogue of the integration on the interval [0, B] is defined as
∫ 0Bμ(t)dqt:=B(1-q)∑j=0∞μ(Bqj)qj,q∈(0,1).
In 1962’s, French engineer Bézier handled the Bernstein basis functions, since they have a simple construction to utilization, to develop the shape design of surface and curve of cars. Moreover, these magnificent polynomials of Bernstein led to many application fields of Mathematics, such as computer graphics, computer-aided geometric design (CAGD), numerical solution of partial differential equations and, etc. Some applications in CAGD, one can refer to [16–19].
In 2019, Cai et al. [20] proposed and studied some statistical approximation properties of a new generalization of (λ,q)-Bernstein polynomials via Bézier bases with shape parameter λ∈[−1,1] as follows:
m≥2,y∈[0,1],0<q≤1,λ∈[−1,1] and bm, j(y; q) are defined in (1).
In the year 2020, Mursaleen et al. [21] considered Chlodowsky kind (λ,q)-Bernstein-Stancu polynomials and derived Korovkin-type convergence, and Voronovskaya-type asymptotic theorems. For some recent relevant works we refer to [22–34].
Motivated by all write above-mentioned works, we will introduce and examine the following Kantorovich version of (λ,q)-Bernstein operators:
Remark 1.1. Let the operators Rm,q,λ(μ;y) be defined by (4). Then,
For λ=0, operators (4) reduce to the Kantorovich type q-Bernstein polynomials constructed by Dalmanoğlu [14].
For λ=0 and q = 1, operators (4) reduce to the classical Kantorovich polynomials [35].
For q = 1, operators (4) reduce to the Kantorovich type λ-Bernstein polynomials proposed by Cai [36].
The present research is organized as follows: In Section 2, we compute several preliminary outcomes such as moments and central moments. In Section 3, we give a Korovkin-type convergence theorem and estimate the degree of convergence in terms of the ordinary modulus of continuity, the functions belong to Lipschitz-type class and Peetre’s K-functional, respectively. In the final section, we demonstrate the comparison of the convergence of operators (4) to a function with some illustrations and error estimation table using Maple software.
Preliminaries
Lemma 2.1. (See [20]) Let eu(t) = tu, u∈N∪{0},y∈[0,1],0<q≤1,λ∈[−1,1] and m > 1. Then, for the operators given by (2) we have
Lemma 2.2. Let y∈[0,1],0<q≤1,λ∈[−1,1] and m > 1. Then, we have
Rm,q,λ(1;y)=1.
Proof. Taking into consideration the definition of q-integral, it follows:
Rm,q,λ(1;y)=[m+1]q∑j=0mb~m,j(y;q,λ)q−j∫[j]q/[m+1]q[j+1]q/[m+1]qdqt=[m+1]q∑j=0mb~m,j(y;q,λ)q−jqj[m+1]q=∑j=0mb~m,j(y;q,λ)=B~m,q,λ(1;y)=1.
Hence, we get (8).
Lemma 2.3 Let y∈[0,1],0<q≤1,λ∈[−1,1] and m > 1. Then, we have
Then,
Rm,q,λ(t;y)=[m+1]q∑j=0mb~m,j(y;q,λ)q−j∫[j]q/[m+1]q[j+1]q/[m+1]qtdqt=[m+1]q∑j=0mb~m,j(y;q,λ)q−jqj[m+1]q2([j]q+11+q)=∑j=0mb~m,j(y;q,λ)[j]q[m+1]q+∑j=0mb~m,j(y;q,λ)1(1+q)[m+1]q=[m]q[m+1]q∑j=0mb~m,j(y;q,λ)[j]q[m]q+1(1+q)[m+1]q∑j=0mb~m,j(y;q,λ)=[m]q[m+1]qB~m,q,λ(t;y)+1(1+q)[m+1]qB~m,q,λ(1;y).
In view of (5) and (6), we obtain desired sequel (9).
Lemma 2.4. Let y∈[0,1],0<q≤1,λ∈[−1,1] and m > 1. Then, we have
By the fact that [j + 1]q = 1+q[j]q, one can has the following easily:
Rm,q,λ(t2;y)=1[m+1]q2∑j=0mb~m,q,λ(y)([j]q2+(2q+1)q2+q+1[j]q+1q2+q+1)=[m]q2[m+1]q2B~m,q,λ(t2;y)+(2q+1)[m]q(q2+q+1)[m+1]q2B~m,q,λ(t;y)+1(q2+q+1)1[m+1]q2B~m,q,λ(1;y).
Then, by (5), (6) and (7), we arrive at (10) so the proof is done.
Corollary 2.1. Let y∈[0,1],0<q≤1,λ∈[−1,1] and m > 1. As a consequence of Lemmas 2.2, 2.3 and 2.4, we arrive the following central moments:
(i)Rm,q,λ(t−y;y)≤qmy[m+1]q+y(1−ym)[m]q−1+2[m]qy[m]q2−1(1+ym[m]q+qy(1−ym−1))+1q[m+1]q([m]q+1)(1+∏r=0m(1−qry)+ym+1+[m+1]qy(1−ym))+[m]q[m+1]q([m]q2−1){2[m+1]qy2(1−ym−1)+2[m+1]qy(1−ym)q[m]q+2q[m]q(1+∏r=0m(1−qry)+ym+1)}+1(1+q)[m+1]q=:αm(y,q).(ii)Rm,q,λ((t−y)2;y)≤q2my2[m+1]q2+[m]qy[m+1]q2(2q+1+(q2+q+1)(1−y)q2+q+1)+2y2(1−ym)[m]q−1+4y2[m]q([m]q2−1)(1+ym[m]q+qy(1−ym−1))+y[m+1]q([m]q−1)(q[m]qy(1−ym−1)+(q2+3q+2)(1−ym)q2+q+1)+2yq[m+1]q([m]q+1)(1+∏r=0m(1−qry)+ym+1+[m+1]qy(1−ym))+1q[m+1]q2([m]q2−1){(3q2+2q+1)[m+1]qy(1−ym)q(q2+q+1)+[m]q[m+1]qy2(1−ym−1)+3q2+2q+1q(q2+q+1)(1+∏r=0m(1−qry)+ym+1)}+2[m]qy[m+1]q([m]q2−1){(q3+3q2+2q+2(q2+q+1)[m+1]qy)(1−ym)q2(q2+q+1)[m]q+q[m−1]q[m+1]qy3(1−ym−2)+(2(q2+q+1)[m+1]qy+q(q3+3q2+5q+1))y(1−ym−1)q2+q+1}+2[m]q[m+1]q2([m]q2−1){(q3+q2+2q+1)[m+1]qy2(1−ym−1)q(q2+q+1)+3q2+2q+1q2(q2+q+1)(1+∏r=0m(1−qry)+ym+1[m]q)+q[m−1]q[m+1]qy3(1−ym−2)+(3q2+q+1)[m+1]qy(1−ym)q2(q2+q+1)}+2y(q+1)[m+1]q+1(q2+q+1)[m+1]q2=:βm(y,q).
Remark 2.1. It can be seen that for a fixed q∈(0,1), m→∞lim[m]q=11−q. In order to provide the convergence results, we get the sequence q: = (qm) such that 0<qm<1,qm→1,1[m]qm→0 as m→∞.
Convergence Results of R\ttextit{m, q, }λ(μ;\ttextit{y})
In this section, we first introduce a Korovkin-type approximation theorem for Rm,q,λ(μ;y). It is a known fact that, the space C[0, 1] denotes the real-valued continuous function on [0, 1] and equipped with the norm for the function μ as ‖μ‖C[0,1]=y∈[0,1]sup|μ(y)|.
Theorem 3.1. Assume that q:={qm} satisfies the conditions as in Remark. Then, for all μ∈C[0,1],λ∈[−1,1],y∈[0,1] and m > 1, we have
m→∞lim‖Rm,qm,λ(μ;.)−μ‖=0.
Proof. Consider the sequence of functions es(y) = ys, where s∈{0,1,2} and y∈[0,1]. According to the Bohman-Korovkin theorem [37], we have to show that
limm→∞‖Rm,qm,λ(es;.)−es‖=0, for s=0,1,2.
The proof of (12) follows easily, using (8), (9) and (10). Hence, we get the required sequel.
Now, we will estimate the order of convergence in terms of the usual modulus of continuity, for the function belong to the Lipschitz type class and the Peetre’s K-functional. By first, we symbolize the usual modulus of continuity of μ∈C[0,1] as follows: ω(μ;η):= 0< a≤ηsupsupy∈[0,1]|μ(y+a)-μ(y)|. Since η>0,ω(μ;η) has some useful properties see details by [38]. Also, we present an element of Lipschitz continuous function with LipL(ζ), where L > 0 and 0<ζ≤1. If the expression below: |μ(t)-μ(y)|≤L|t-y|ζ,(t,y∈ℝ), holds, then one can say μ is belong to LipL(ζ).
Also, the Peetre’s K-functional is defined byK2(μ,η)= infν∈C2[0,1]{∥μ-ν∥+η∥ν′′∥}, where η>0 and C2[0,1]={ν∈C[0,1]:ν′,ν′′∈C[0,1]}.
Taking into account [39], there exists an absolute constant C > 0 such that
K2(μ;η)≤Cω2(μ;η),η>0
where ω2(μ;η)= 0< z≤ηsupsupy∈[0,1]|μ(y+2z)-2μ(y+z)+μ(y)|, is the second order modulus of smoothness of μ∈C[0,1].
Theorem 3.2. Assume that q:={qm} satisfies the conditions as in Remark 2.1. Then, for all μ∈C[0,1],λ∈[−1,1],y∈[0,1] and m > 1, we obtain |Rm,qm,λ(μ;y)-μ(y)|≤2ω(μ;βm(y,qm)), where βm(y,qm)=Rm,qm,λ((t−y)2;y) same as in Corollary 2.1.
Proof. Taking |μ(t)−μ(y)|≤(1+|t−y|δ)ω(μ;δ) into account and after operating Rm,qm,λ(.;y), we get |Rm,qm,λ(μ;y)-μ(y)|≤(1+1δRm,qm,λ(|t-y|;y))ω(μ;δ). Utilizing the Cauchy-Bunyakovsky-Schwarz inequality, it follows:
|Rm,qm,λ(μ;y)−μ(y)|≤(1+1δRm,qm,λ((t−y)2;y))ω(μ;δ)≤(1+1δβm(y,qm))ω(μ;δ).
Choosing δ=βm(y,qm), which completes the proof.
Theorem 3.3. Assume that q:={qm} satisfies the conditions as in Remark 2.1. Then, for all μ∈LipL(ζ),0<ζ≤1,y∈[0,1], λ∈[−1,1] and m > 1, we obtain |Rm,qm,λ(μ;y)-μ(y)|≤L(βm(y,qm))ζ2.
Proof. Let μ∈LipL(ζ). Using the linearity and monotonicity properties of the operators (4), therefore
|Rm,qm,λ(μ;y)−μ(y)|≤Rm,qm,λ(|μ(t)−μ(y)|;y)=[m+1]qm∑j=0mb~m,qm,λ(y)qm−j∫[j]qm/[m+1]qm[j+1]qm/[m+1]qm|μ(t)−μ(y)|dqmt≤L([m+1]qm∑j=0mb~m,qm,λ(y)q−j∫[j]qm/[m+1]qm[j+1]qm/[m+1]qm|t−y|ζdqmt).
Using the Hölder’s inequality and with p1=2ζ and p2=22−ζ, one has 1p1+1p2=1. Hence, we may write
|Rm,qm,λ(μ;y)−μ(y)|≤L([m+1]qm∑j=0mb~m,qm,λ(y)q−j∫[j]qm/[m+1]qm[j+1]qm/[m+1]qm|t−y|2dqmt)ζ2≤L(Rm,qm,λ((t−y)2;y))ζ2≤L(βm(y,qm))ζ2.
Hence, Theorem 3.3 is proved.
Theorem 3.4. For all μ∈C[0,1],y∈[0,1] and λ∈[−1,1], the following inequality holds true |Rm,q,λ(μ;y)-μ(y)|≤Cω2(μ;12βm(y,q)+(αm(y,q))2)+ω(μ;αm(y,q)), where C > 0 is a positive constant, αm(y,q) and βm(y,q) are same as in Corollary 2.1.
Proof. Firstly, we define the following auxiliary operators:
After operating R^m,q,λ(.;y) to (15), yields
R^m,q,λ(ξ;y)−ξ(y)=R^m,q,λ((t−y)ξ′(y);y)+R^m,q,λ(∫ty(t−u)ξ′′(u)du;y)=ξ′(y)R^m,q,λ(t−y;y)+Rm,q,λ(∫ty(t−u)ξ′′(u)du;y)−∫Rm,q,λ(t;y)y(Rm,q,λ(t;y)−u)ξ′′(u)du=Rm,q,λ(∫ty(t−u)ξ′′(u)du;y)−∫Rm,q,λ(t;y)y(Rm,q,λ(t;y)−u)ξ′′(u)du.
Considering (14), we get
|R^m,q,λ(ξ;y)−ξ(y)|≤|Rm,q,λ(∫ty(t−u)ξ′′(u)du;y)|+|∫yRm,q,λ(t;y)(Rm,q,λ(t;y)−u)ξ′′(u)du|≤Rm,q,λ(|∫yt(t−u)||ξ′′(u)||du|;y)+∫yRm,q,λ(t;y)|Rm,q,λ(t;y)−u||ξ′′(u)||du|≤‖ξ′′‖{Rm,q,λ((t−y)2;y)+(Rm,q,λ(t;y)−y)2}≤{βm(y,q)+(αm(y,q))2}‖ξ′′‖.
On the other hand using (8), (9) and (14), it deduce the following:
With the help of (15) and (16), we get
|Rm,q,λ(μ;y)−μ(y)|≤|R^m,q,λ(μ−ξ;y)−(μ−ξ)(y)|+|R^m,q,λ(ξ;y)−ξ(y)|+|μ(y)−μ(Rm,q,λ(t;y))|≤4‖μ−ξ‖+{βm(y,q)+(Rm,q,λ(t;y))2}‖ξ′′‖+ω(μ;αm(y,q)).
On account of this, if we take the infimum on the right hand side over all ξ∈C2[0,1] and in view of (13), we arrive
|Rm,q,λ(μ;y)−μ(y)|≤4K2(μ;{βm(y,q)+(αm(y,q))2}4)+ω(μ;αm(y,q))≤Cω2(μ;12βm(y,q)+(αm(y,q))2)+ω(μ;αm(y,q)).
Hence, we obtain the proof of this theorem.
Graphical and Numerical Examples
In this section, we present some graphics and error estimation table to see the convergence behaviour of Rm,q,λ(μ;y) operators to a function.
Example. Consider the function
μ(y)=1−sin(πy)
on the interval [0, 1].
In Fig. 1, we demonstrate the approximations of Rm,q,1(μ;y) and Rm,q,−1(μ;y) operators to μ(y) for different values of m and q.
In Fig. 2, we show the approximations of Rm,q,0(μ;y) and Rm,q,1(μ;y) operators to μ(y) for m = 10 and q = 0.9.
Also, in Table 1, we calculate the maximum error of approximation of Rm,q,λ(μ;y) operators for some values of m, q and λ in view of μ(y).
The convergence of Rm,q,λ(μ;y) operators to μ(y)=1−sin(πy) for λ=1, λ=−1 and different values of m and q
The convergence of Rm,q,λ(μ;y) operators to μ(y)=1−sin(πy) for λ=0, λ=1, m = 10 and q = 0.9
Error of approximation Rm,q,λ(μ;y) operators to μ(y)=1−sin(πy) for different values of m, q and λ
λ
q
|μ(y)−Rm,q,λ(μ;y)|
m = 15
m = 45
m = 125
0.9
0.1272102421
0.1091438514
0.1084604470
1
0.99
0.0747917138
0.0320712502
0.0168560799
0.999
0.0705273105
0.0266032428
0.0102987106
0.9
0.1305031803
0.1106365735
0.1099013419
0
0.99
0.0761998009
0.0321428950
0.0168623572
0.999
0.0718123066
0.0266565471
0.0103014327
0.9
0.1337961186
0.1121292958
0.1113422366
−1
0.99
0.0776078880
0.0322145398
0.0168686344
0.999
0.0730973026
0.0267098514
0.0103041547
It is obvious from Table 1 that, in case λ=1 and as the value m increases than the absolute error bounds of |μ(y)−Rm,q,1(μ;y)| are smaller than |μ(y)−Rm,q,0(μ;y)|. Namely, our newly defined operators (4), in case λ>0 has better approximation than Kantorovich type q-Bernstein polynomials.
Conclusion
In this work, we introduced a Kantorovich type of q-Bernstein operators based on the Bézier basis functions with shape parameter λ∈[−1,1]. Due to the parameter λ, we have more flexibility in modeling. Some approximation properties of these operators such as a Korovkin type convergence theorem and as well as the order of convergence concerning with the usual modulus of continuity, Lipschitz-type functions and Peetre’s K-functional are studied. Moreover, we made our work more intuitive by using some graphs and error estimation table. As future works, we may consider Durrmeyer and Stancu kinds of q-Bernstein operators with shape parameter λ.
Authors Contributions: The authors contributed equally and significantly in writing this paper. All authors read and approved the final manuscript.
Acknowledgement: We thank Fujian Provincial Big Data Research Institute of Intelligent Manufacturing of China.
Funding Statement: This work is supported by the Natural Science Foundation of Fujian Province of China (Grant No. 2020J01783), the Project for High-Level Talent Innovation and Entrepreneurship of Quanzhou (Grant No. 2018C087R) and the Program for New Century Excellent Talents in Fujian Province University.
Conflicts of Interest: The authors declare that they have no conflicts of interest to report regarding the present study.
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