Return to Article Details A Stancu type extension of the Campiti-Metafune operator

A Stancu type extension
of the Campiti-Metafune operator

Teodora Cătinaş∗
(Date: November 01, 2025; accepted: November 21, 2025; published online: December 22, 2025.)
Abstract.

We consider an extension of the Campiti-Metafune operator using a Stancu type technique. We study some properties of the new obtained operator.

Key words and phrases:
Campiti-Metafune operator, Stancu operator, Bernstein operator, moments of the operator.
2005 Mathematics Subject Classification:
41A10, 41A35, 41A36, 47A58.
∗Babeş-Bolyai University, Faculty of Mathematics and Computer Science, Str. M. Kogălniceanu Nr. 1, RO-400084 Cluj-Napoca, Romania, e-mail: teodora.catinas@ubbcluj.ro.

1. Introduction

In 1982, D.D. Stancu [6], introduced a new Bernstein type operator given by

(1) Ln,r⁢(f;x)=∑k=0n−rbn−r,k⁢(x)⁢[(1−x)⁢f⁢(kn)+x⁢f⁢(k+rn)],

where bn,k denote the basis Bernstein polynomials of degree n,

bn,k=(nk)⁢xk⁢(1−x)n−k⁢, ⁢k=0,1,…,n,

for f∈C⁢[0,1], n,r∈ℕ such that n>2⁢r.

In 1996, M. Campiti and G. Metafune [3], introduced and studied a new Bernstein type operator that now bears their names. For introducing the operator, we need two sequences λ=(λn)n≥1 and ρ=(ρn)n≥1, and the numbers αn,k defined by

(2) αn,0=λn,αn,n=ρn,αn+1,k=αn,k+αn,k−1,for ⁢k=1,n¯,n∈ℕ.

The Campiti-Metafune operator An:C⁢([0,1])→C⁢([0,1]), is given by [3]

(3) (An⁢f)⁢(x)=∑k=0nαn,k⁢xk⁢(1−x)n−k⁢f⁢(kn).
Remark 1.

If λ and ρ are constant sequences of term 1, then αn,k=(nk), for k=0,n¯ and An becomes Bernstein operator Bn, given by

(Bn⁢f)⁢(x)=∑k=0n(nk)⁢xk⁢(1−x)n−k⁢f⁢(kn).

For the sequences (λ,ρ) we consider the following choices, as in [1]:

(i) Case λ=δm, m∈ℕ, ρ=0, where δm=(δn,m)n≥1, δn,m={1,n=m0,n≠m. We denote An(δm,0) by Lm,n and it is called the elementary left operator of order m associated to An.

The coefficients of the operators Lm,n are denoted by lm,n,k and they are defined by

lm,n,k={0,(n<m)⁢ or(n=m,k≥1)(n>m,k=0)(n>m,k≥n−m+1)1,n=m,k=0(n−m−1k−1),n>m,1≤k≤n−m..

(ii) Case λ=0, ρ=δm, m∈ℕ. We denote An(0,δm) by Rm,n and it is called elementary right operator of order m associated to An.

The coefficients of the operators Rm,n are denoted by rm,n,k and they are defined by

rm,n,k={0,(n<m)⁢ or(n=m,k≤n−1)(n>m,k≤m−1)(n>m,k=n)1,n=m,k=n(n−m−1k−m),n>m,m≤k≤n−1..

Consequently, for any (m,n)∈ℕ×ℕ we get

(4) (Lm,n⁢f)⁢(x)=∑k=1n−mam,n,k⁢(x)⁢f⁢(kn),

with

(5) am,n,k⁢(x)=(n−m−1k−1)⁢xk⁢(1−x)n−k,

for m<n and

(Ln,n⁢f)⁢(x)=(1−x)n⁢f⁢(0).

We have

(6) (Rm,n⁢f)⁢(x)=∑k=mn−1bm,n,k⁢(x)⁢f⁢(kn),

with

(7) bm,n,k⁢(x)=(n−m−1k−m)⁢xk⁢(1−x)n−k,

for m<n and

(Rn,n⁢f)⁢(x)=xn⁢f⁢(1).

Using these elementary operators, the operator An is decomposed as

(8) An=∑m=1nλm⁢Lm,n+∑m=1nρm⁢Rm,n.
Remark 2.

For the particular case of λ=ρ=1, we get

Bn=∑m=1n(Lm,n+Rm,n).

2. A Stancu type extension of the Campiti-Metafune operator

Now we introduce the Stancu type extension of the Campiti-Metafune operator, based on an idea from [2], also used, for example, in [4], [5]. Using the Stancu type operator (1) and the operator (8), we get

(9) (AnS⁢f)⁢(x):=∑m=1nλm⁢(Lm,n,rS⁢f)⁢(x)+∑m=1nρm⁢(Rm,n,rS⁢f)⁢(x)

with

(Lm,n,rS⁢f)⁢(x)=∑k=1n−m−ram,n−r,k⁢(x)⁢[(1−x)⁢f⁢(kn)+x⁢f⁢(k+rn)]

and

(Rm,n,rS⁢f)⁢(x)=∑k=mn−r−1bm,n−r,k⁢(x)⁢[(1−x)⁢f⁢(kn)+x⁢f⁢(k+rn)],

where am,n−r,k⁢(x) and bm,n−r,k⁢(x) are given by (5) and (7), for f∈C⁢[0,1] and n,r∈ℕ such that n>2⁢r.

Remark 3.

For r=0, it is obtained AnS as the Campiti-Metafune operator An.

We are going to calculate the moments of the new operators and to study some approximation properties.

3. Properties of the Campiti-Metafune operator

We give first some results regarding the Campiti-Metafune operator that will be used in the sequel in order to prove some properties of the new constructed operator.

Lemma 4 ([1]).

The operators defined by (4) and (6) verify the following relations:

1∘

(Lm,n⁢e0)⁢(x)={x⁢(1−x)m,n>m;(1−x)n,n=m;

(Rm,n⁢e0)⁢(x)={(1−x)⁢xm,n>m;xn,n=m;

2∘
(Lm,n⁢e1)⁢(x)={x⁢(1−x)m⁢(1+(n−m−1)⁢x)n,n>m;0,n=m;
(Rm,n⁢e1)⁢(x)={(1−x)⁢xm⁢(m+(n−m−1)⁢x)n,n>m;xn,n=m;

3∘
(Lm,n⁢e2)⁢(x)={x⁢(1−x)m⁢1+3⁢(n−m−1)⁢x+(n−m−1)⁢(n−m−2)⁢x2n2,n>m;0,n=m;
(Rm,n⁢e2)⁢(x)={(1−x)⁢xm⁢m2+(1+2⁢m)⁢(n−m−1)⁢x+(n−m−1)⁢(n−m−2)⁢x2n2,n>m;xn,n=m.

Now we study some properties for the new operator, AnS introduced in (9).

Theorem 5.

For every x∈[0,1], n,r∈ℕ such that n>2⁢r, we have the following results:

i)

(AnS⁢e0)⁢(x) =∑m=1nλm⁢(Lm,n,rS⁢e0)⁢(x)+∑m=1nρm⁢(Rm,n,rS⁢e0)⁢(x)
=∑m=1n−r−1(λm⁢x⁢(1−x)m+ρm⁢xm⁢(1−x))+λn−r⁢(1−x)n−r+ρn−r⁢xn−r

ii)

(AnS⁢e1)⁢(x):=∑m=1nλm⁢(Lm,n,rS⁢e1)⁢(x)+∑m=1nρm⁢(Rm,n,rS⁢e1)⁢(x)

iii)

(AnS⁢e2)⁢(x):=∑m=1nλm⁢(Lm,n,rS⁢e2)⁢(x)+∑m=1nρm⁢(Rm,n,rS⁢e2)⁢(x)

with

(Lm,n,rS⁢e0)⁢(x)={x⁢(1−x)m,n>m+r;(1−x)n−r,n=m+r;
(Rm,n,rS⁢e0)⁢(x)={(1−x)⁢xm,n>m+r;xn−r,n=m+r;,

and

(Lm,n,rS⁢e1)⁢(x)={x⁢(1−x)m⁢(1+(n−r−m−1)⁢x)n−r+rn⁢x2⁢(1−x)m,n>m+r;rn⁢x⁢(1−x)n−r,n=m+r;
(Rm,n,rS⁢e1)⁢(x)={(1−x)⁢xm⁢(m+(n−r−m−1)⁢x)n−r+rn⁢x⁢(1−x)⁢xm,n>m+r;xn−r+rn⁢xn−r+1,n=m+r;

and

(Lm,n,rS⁢e2)⁢(x)⁢(x)=
={x⁢(1−x)m⁢{1+3⁢(n−r−m−1)⁢x+(n−r−m−1)⁢(n−r−m−2)⁢x2}(n−r)2+2⁢rn⁢x2⁢(1−x)m⁢(1+(n−r−m−1)⁢x)n−r+r2n2⁢x3⁢(1−x)m,n>m+r;r2n2⁢x⁢(1−x)n−r,n=m+r;
(Rm,n,rS e2)(x)(x)=
={(1−x)⁢xm⁢m2+(1+2⁢m)⁢(n−r−m−1)⁢x+(n−r−m−1)⁢(n−r−m−2)⁢x2(n−r)2+2⁢rn⁢x⁢(1−x)⁢xm⁢(m+(n−r−m−1)⁢x)n−r+r2⁢x2n2⁢(1−x)⁢xm,n>m+r;xn−r+2⁢rn⁢xn−r+1+r2⁢x2n2⁢xn−r,n=m+r;
Proof.
(10) (AnS⁢e0)⁢(x):=∑m=1nλm⁢(Lm,n,rS⁢e0)⁢(x)+∑m=1nρm⁢(Rm,n,rS⁢e0)⁢(x)

with

(Lm,n,rS⁢e0)⁢(x) =∑k=1n−m−ram−r,n,k⁢(x)=(Lm,n−r⁢e0)⁢(x)
={x⁢(1−x)m,n>m+r;(1−x)n−r,n=m+r;

and

(Rm,n,rS⁢e0)⁢(x) =∑k=mn−r−1bm−r,n,k⁢(x)=(Rm,n−r⁢e0)⁢(x)
={(1−x)⁢xm,n>m+r;xn−r,n=m+r;.

So, we have

(AnS⁢e0)⁢(x):=∑m=1nλm⁢(Lm,n−r⁢e0)⁢(x)+∑m=1nρm⁢(Rm,n−r⁢e0)⁢(x)=(An−r⁢e0)⁢(x)

By (10) we get

(AnS⁢e0)⁢(x)=∑m=1n−r−1(λm⁢x⁢(1−x)m+ρm⁢xm⁢(1−x))+λn−r⁢(1−x)n−r+ρn−r⁢xn−r

ii) We have

(AnS⁢e1)⁢(x):=∑m=1nλm⁢(Lm,n,rS⁢e1)⁢(x)+∑m=1nρm⁢(Rm,n,rS⁢e1)⁢(x)

with

(Lm,n,rS⁢e1)⁢(x) =∑k=1n−m−ram,n−r,k⁢(x)⁢[(1−x)⁢kn+x⁢k+rn]
=(Lm,n−r⁢e1)⁢(x)+rn⁢x⁢(Lm.n−r⁢e0)⁢(x)

and

(Rm,n,rS⁢e1)⁢(x) =∑k=mn−r−1bm,n−r,k⁢(x)⁢[(1−x)⁢kn+x⁢k+rn]
=(Rm,n−r⁢e1)⁢(x)+rn⁢x⁢(Rm.n−r⁢e0)⁢(x)

and by Lemma 4, we get

(Lm,n,rS⁢e1)⁢(x)⁢(x) =(Lm,n−r⁢e1)+rn⁢x⁢(Lm.n−r⁢e0)⁢(x)
={x⁢(1−x)m⁢(1+(n−r−m−1)⁢x)n−r+rn⁢x2⁢(1−x)m,n>m+r;rn⁢x⁢(1−x)n−r,n=m+r;

and

(Rm,n,rS⁢e1)⁢(x) =(Rm,n−r⁢e1)⁢(x)+rn⁢x⁢(Rm.n−r⁢e0)⁢(x)
={(1−x)⁢xm⁢(m+(n−r−m−1)⁢x)n−r+rn⁢x⁢(1−x)⁢xm,n>m+r;xn−r+rn⁢xn−r+1,n=m+r;

iii) We have

(AnS⁢e2)⁢(x):=∑m=1nλm⁢(Lm,n,rS⁢e2)⁢(x)+∑m=1nρm⁢(Rm,n,rS⁢e2)⁢(x)

with

(Lm,n,rS⁢e2)⁢(x)⁢(x) =∑k=1n−m−ram,n−r,k⁢(x)⁢[(1−x)⁢k2n2+x⁢(k+r)2n2]
=(Lm,n−r⁢e2)⁢(x)+2⁢rn⁢x⁢(Lm.n−r⁢e1)⁢(x)+r2⁢x2n2⁢(Lm.n−r⁢e0)⁢(x)

and

(Rm,n,rS⁢e2)⁢(x)⁢(x) =∑k=1n−m−ram,n−r,k⁢(x)⁢[(1−x)⁢k2n2+x⁢(k+r)2n2]
=(Rm,n−r⁢e2)⁢(x)+2⁢rn⁢x⁢(Rm.n−r⁢e1)⁢(x)+r2⁢x2n2⁢(Rm.n−r⁢e0)⁢(x).

By Lemma 4, we get

(Lm,n,rS⁢e2)⁢(x)⁢(x)=
=(Lm,n−r⁢e2)⁢(x)+2⁢rn⁢x⁢(Lm.n−r⁢e1)⁢(x)+r2⁢x2n2⁢(Lm.n−r⁢e0)⁢(x)
={x⁢(1−x)m⁢1+3⁢(n−r−m−1)⁢x+(n−r−m−1)⁢(n−r−m−2)⁢x2(n−r)2+2⁢rn⁢x⁢x⁢(1−x)m⁢(1+(n−r−m−1)⁢x)n−r+r2n2⁢x3⁢(1−x)m,n>m+r;r2n2⁢x2⁢(1−x)n−r,n=m+r;

and

(Rm,n,rS⁢e2)⁢(x)⁢(x)=
=(Rm,n−r⁢e2)⁢(x)+2⁢rn⁢x⁢(Rm.n−r⁢e1)⁢(x)+r2⁢x2n2⁢(Rm.n−r⁢e0)⁢(x)
={(1−x)⁢xm⁢m2+(1+2⁢m)⁢(n−r−m−1)⁢x+(n−r−m−1)⁢(n−r−m−2)⁢x2(n−r)2+2⁢rn⁢x⁢(1−x)⁢xm⁢(m+(n−r−m−1)⁢x)n−r+r2⁢x2n2⁢(1−x)⁢xm,n>m+r;xn−r+2⁢rn⁢xn−r+1+r2⁢x2n2⁢xn−r,n=m+r;

∎

Theorem 6.

For every f∈C⁢[0,1], we have

‖Lm,n,rS‖≤‖f‖⁢ and ⁢‖Rm,n,rS‖≤‖f‖.
Proof.

Considering the expression of Lm,n,rS⁢f and Rm,n,rS⁢f, and Lemma 4, we get

|(Lm,n,rS⁢f)⁢(x)| =|∑k=1n−m−ram,n−r,k⁢(x)⁢[(1−x)⁢f⁢(kn)+x⁢f⁢(k+rn)]|
≤∑k=1n−m−ram,n−r,k⁢(x)⁢|[(1−x)⁢f⁢(kn)+x⁢f⁢(k+rn)]|
≤∑k=1n−m−ram,n−r,k⁢(x)⁢[(1−x)⁢|f⁢(kn)|+x⁢|f⁢(k+rn)|]
≤‖f‖⁢∑k=1n−m−ram,n−r,k⁢(x)
≤‖f‖⁢(Lm,n,rS⁢e0)⁢(x)
≤‖f‖
|(Rm,n,rS⁢f)⁢(x)| =|∑k=mn−r−1bm,n−r,k⁢(x)⁢[(1−x)⁢f⁢(kn)+x⁢f⁢(k+rn)]|
≤∑k=1n−m−rbm,n−r,k⁢(x)⁢|[(1−x)⁢f⁢(kn)+x⁢f⁢(k+rn)]|
≤∑k=1n−m−rbm,n−r,k⁢(x)⁢[(1−x)⁢|f⁢(kn)|+x⁢|f⁢(k+rn)|]
≤‖f‖⁢(Rm,n,rS⁢e0)⁢(x)
≤‖f‖

∎

References