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Research article

On the Fractal interpolation functions associated with Matkowski contractions

  • Received: 04 April 2023 Revised: 01 June 2023 Accepted: 15 June 2023 Published: 29 June 2023
  • In this paper we investigate an iterated function system that defines a fractal interpolation function, where ordinate scaling, that is Lipschitz constant in Banach contraction principle is substituted by real-valued control function. In such a manner, fractal interpolation functions associated with Matkowski contractions are obtained and provide a new framework of approximating experimental data. Furthermore, given a data generating function f, we study a new class of fractal interpolation functions which converge to f.

    Citation: Najmeddine Attia, Mohamed balegh, Rim Amami, Rimah Amami. On the Fractal interpolation functions associated with Matkowski contractions[J]. Electronic Research Archive, 2023, 31(8): 4652-4668. doi: 10.3934/era.2023238

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  • In this paper we investigate an iterated function system that defines a fractal interpolation function, where ordinate scaling, that is Lipschitz constant in Banach contraction principle is substituted by real-valued control function. In such a manner, fractal interpolation functions associated with Matkowski contractions are obtained and provide a new framework of approximating experimental data. Furthermore, given a data generating function f, we study a new class of fractal interpolation functions which converge to f.



    Fractal methodology provides a general frame for the understanding of real-world phenomena. In particular, fractal interpolation techniques, defined as fixed points of maps between spaces of functions using iterated function system prove to be more general than classical interpolants and provide good deterministic representations of complex phenomena. Indeed, the fractal interpolation function is not necessarily differentiable at any point, thus, it is closer to natural world phenomena and provides a more powerful tool in fitting real-world data compared to other types of interpolation techniques. In the following, we will recall the iterated function system model which is based upon the property of self-similarity which stipulates that the shape resembles the whole irrespective to the degree of magnification.

    Let (X,d) be a complete metric space and let H(X) be the set of nonempty compact subsets of X. We define the Hausdorff metric dH by

    dH(A,B)=max{D(A,B),D(B,A)},A,BH(X),

    with

    D(A,B)=supxAinfyBd(x,y) and D(B,A)=supxBinfyAd(x,y).

    The space (H(X),dH) is complete, and compact whenever X is compact [1]. Let NN, the set of positive integers, and wn:XX be a continuous map, n=1,,N. Then

    I={X,w1,w2,,wN}

    is called an iterated function system (IFS in short). Now, we define the Hutchinson operator W:H(X)H(X) by

    W(B)=Nn=1wn(B), BH(X), (1.1)

    where wn(B)={wn(x), xB}. For kN, let Wk denote the k-fold auto composition of W. Any set GH(X) such that W(G)=G is called an attractor for the IFS and the IFS admits always at least one attractor [2]. Moreover, if each wn is a contraction, i.e., if there exists c[0,1) such that d(w(x),w(y))cd(x,y), for all x,yX then I is called hyperbolic. In this case the Hutchinson operator W is a contraction mapping, that is,

    dH(W(A),W(B))cdH(A,B)A,BH(X)

    and then admits a unique attractor G=limkWk(B), for an arbitrary BH(X) [2]. The classical framework of IFS was studied in [1,3,4] as a finite set of contraction maps defined on a compact set of a Euclidean space Rn. Since then, many researchers have been working on extending these results to more general spaces, generalized contractions and infinite IFSs ([5,6,7,8,9]).

    The fixed point theory plays an important role for the existence of invariant sets in different types of IFSs and this is done by considering a suitable map. In particular, fractal interpolation functions, as an alternative to classical interpolation such as polynomial interpolation, arise as fixed points of the Read-Bajraktarević operator defined on suitable function spaces. This concept was first introduced in 1986 by Barnsley [2] to interpolate a given set of data points. Since then, the theory of fractal interpolation has become a powerful and useful tool in applied sciences and engineering. In addition, various types of fractal interpolation functions have been constructed and some of their significant properties including calculus, dimension, smoothness, stability, perturbation error, etc, have been widely studied ([10,11,12,13]). The problem of the existence of the fractal interpolation function (FIF) returns to the study of the existence (and uniqueness) of some fixed points on the fractal space. The most widely studied FIFs are based on the Banach fixed point theorem. This classical result has been extended in several ways, and recently, many researchers have studied the existence of FIFs by using different well-known fixed point results obtained in the fixed point theory [15,16]. In particular in [17] the authors ensure that the attractor of a nonlinear IFS constructed by Geraghty contractions are graphs of some continuous functions which interpolate the given data and in [18] the authors investigate Branciari contraction. In this paper, we investigate Matkowski contractions, introduced in [19].

    Definition 1. Let φ:[0,)[0,) and f:XX be a map. We say that

    1) f is φ-contraction if

    d(f(x),f(y))φ(d(x,y))

    for all x,yX.

    2) f is Matkowski contraction if it is a φ-contraction where the function φ is non-decreasing and the limnφn(t)=0 for all t>0.

    In particular, each Banach contraction is a Matkowski contraction with φ(t)=Ct. In addition, we have the following result.

    Theorem 1. [19] Let (X,d) be a complete metric space. If the function f:XX is a Matkowski contraction, then f has a unique fixed point x0X. Moreover, for every xX, we have limnfn(x)=x0.

    This result may be seen as a generalization of the Banach theorem [20]. Take, for example, X=[0,1] endowed with the Euclidean metric and consider the function f(x)=2x2+x. Then, it is easy to see that the mapping f is not a Banach contraction, indeed,

    supxy|f(x)f(y)||xy|=supxy4(2+x)(2+y)=1.

    Moreover, for all x,y0, we have

    d(f(x),f(y))4|xy)(2+x)(2+y)|xy|1+|xy|

    It follows that f is a Matkowski contraction with comparison function φ(t)=t1+t.

    In the present work, we will first construct a generalized iterated function systems (GIFS in short). The framework of GIFS was introduced by Mihail and Miculescu [7,21] as a natural generalization of a classical IFS. More precisely, GIFS consists of mappings f:XmX, for m>1, instead of self-mappings of a metric space X, where Xm is the Cartesian product of m copies of X. Since then, it has been the subject of study of several papers [8,22,23,24,25]. Let J={1,,N} and, for each nJ, let fn be a Matkowski contraction. In Section 2, we give a quick proof of the fact that the GIFS {Xm, fn, nJ} admits a unique attractor. Moreover, for m=1, we ensure that attractors of IFSs constructed by using a Matkowski contraction are graphs of some continuous functions which interpolate the given data. This result is a generalization of the result given in [17] since each Geraghty contraction is a Matkowski contraction (see [26] for comparison on these two contractions).

    Let C(I) be the set of continuous functions over the interval I. Using a fractal interpolation function through a suitable IFS, we can define a method to perturb a function fC(I). We obtain, for free parameter α, usually called scale vector, a class of functions fαC(I) which interpolate and approximate simultaneously the function f. Moreover, we can select a suitable IFS so that the corresponding fractal function fα shares the quality of smoothness or non-smoothness of f or preserves fundamental shape properties, namely positivity, monotonicity, and convexity [27,28]. In Section 3, we study a new class of fractal interpolation functions which converges to f.

    Let mN and f:XmX be a mapping, where the product space is endowed with the metric denoted also by d and defined by

    d((x1,,xm),(y1,,ym))=max{d(x1,y1),,d(xm,ym)}, (2.1)

    for all (x1,,xm), (y1,,ym)Xm. The mapping f is said to be a Matkowski contraction if, for all j{1,,m}, f is φ-contraction, that is,

    d(f(u),f(v))φ(d(xj,yj)) (2.2)

    for all u=(x1,,xm),v=(y1,,ym)Xm, where the function φ is non-decreasing and the limnφn(t)=0 for all t>0. Many types of φ-contractions in the literature are considered, see for example, Rakotch contraction [29] and Browder contraction [30]. In addition, it is worth mentioning that the earlier observation shows that, among compact spaces, the notions of Matkowski, Browder and Rakotch contractions coincide [26].

    We say that f has a unique fixed point if there exists a unique xX such that f(x,x,,x)=x. Any mapping f from (X,d) to itself, that is m=1, satisfying (2.2) has a unique fixed point (Theorem 1). In this section we will prove that, if f is a Matkowski contraction, then f has a unique fixed point. Therefore, we may define a GIFS which admits a unique attractor. Our first result in this section is the following.

    Proposition 1. Let (X,d) be a complete metric space and mN. Assume that the mapping f:XmX is a Matkowski contraction, satisfying (2.2), then f has a unique fixed point.

    Proof. Assume that m>1 and let g:XX be a mapping such that g(x)=f(x,,x), for all xX. Using (2.2), we get

    d(g(x),g(y))φ(d(x,y)),

    for all x,yX. It follows, that g is a Matkowski contraction and then, by Theorem 1, the mapping g has a unique fixed point aX. Whence (a,,a) is the unique fixed point of f.

    Example 1. Let m=2 and X=[0,1]{4} be a metric space endowed with the Euclidean metric. We define the functions

    f(x,y)={x/2,x,y[0,1]12y1+y,x=4,y40,y=4φ(t)={t2,t[0,1]t21+t,t>1

    In the following we will verify the inequality (2.2). For this, we will consider five possible cases. Let u=(x,y)X and v=(x,y)X. First remark that the case y=y=4 is trivial so we will assume that (y,y)(4,4).

    Case 1: f(u)=x/2 and f(v)=x/2. This is the case when u,v[0,1]2 and then

    d(f(u),f(v))=12|xx|φ(d(u,v))

    Case 2: f(u)=12y1+y and f(v)=0. This is the case when x=y=4 and y4 (the case when f(v)=12y1+y and f(u)=0 is similar). In this case, we have

    d(f(u),f(v))12y1+y12.

    Note that the function ϕ is strictly increasing on (1,+) and

    φ(x)>12,x>1. (2.3)

    Therefore, since |yy|>2, we obtain d(f(u),f(v))φ(d(u,v)).

    Case 3: f(u)=12y1+y and f(v)=12y1+y. This is the case when x=x=4, y4 and y4. Then,

    d(f(u),f(v))12|yy|=φ(d(u,v))

    Case 4: f(u)=x/2 and f(v)=0. This is the case when x4, y4 and y=4 (the case f(v)=x/2 and f(u)=0 is similar). It follows, using (2.3), then

    d(f(u),f(v))12φ(d(u,v))

    Case 5: f(u)=x/2 and f(v)=12y1+y. This is the case when x,y4, x=4 and y4 (the case f(v)=x/2 and f(u)=12y1+y is similar). Then,

    d(f(u),f(v))=|x212y1+y|12φ(d(u,v))

    Let, for n=1,,N, fn:XmX be a Matkowski contraction mapping. Then

    I={Xm,f1,f2,,fN}

    is called a GIFS. Now, we define the fractal operator F:H(X)mH(X), associated with the GIFS, by

    F(B1,B2,,Bm)=Nn=1fn(B1,B2,,Bm). (2.4)

    Any fixed point of the operator F, that is, a set GH(X) such that F(G,G,,G)=G is called an attractor for the GIFS. In the next section, we prove that any GIFS satisfying the Matkowski contraction admits a unique attractor G [24, Theorem 4].

    Theorem 2. Let (X,d) be a complete metric space and we define, for nJ, the mappings fn:XmX satisfying the Matkowski contraction (2.2) with the same function φ. Then the GIFS {Xm, fn, nJ} admits a unique attractor G.

    Proof. Let A=(A1,,Am) and B=(B1,,Bm)H(X)m. Choose j{1,,m} and let φ such that (2.2) is satisfied for the mappings fn, nJ. We only have to prove that

    dH(F(A),F(B))φ(dH(Aj,Bj)) (2.5)

    from which we deduce that the fractal operator F is a Matkowski contraction on (H(Xm),dH). Using Proposition 1, F has a unique fixed point G as required.

    Let zF(A1,,Am), then there exists nJ such that z=fn(x1,,xm) with xiAi, for all iJ. Now, since Bj is compact, then there exists yjBj such that

    d(xj,yj)=infyBjd(xj,y).

    Therefore d(xj,yj)D(Aj,Bj)dH(Aj,Bj). It follows that

    d(z,F(B1,,Bm)d(z,fn(B1,,Bm))d(fn(x1,,xm),fn(y1,,ym))φ(dH(Aj,Bj)).

    Remark that F(A) is a compact set of H(X)m and zd(z,F(B)) is continuous. Therefore

    D(F(A),F(B)))φ(dH(Aj,Bj)).

    Similarly, we may prove that D(F(B),F(A))φ(dH(Aj,Bj)) and then (2.5).

    Let Δ:x0<x1<<xN be a partition of the real compact interval I=[x0,xN] and consider the data set {(xi,yi)I×Ri=0,1,,N}. Let K be a suitable compact subset of R containing yi, iJ0={0,,N}. We assume that the compact metric space I×K is endowed with uniform metric d defined as

    d((x1,y1),(x2,y2))=max{|x1x2|,|y1y2|},

    for all (x1,x2)I2 and (y1,y2)K2. Recall the set J={1,,N} introduced in the Section 1. For iJ, we set Ii=[xi1,xi] and let Li:IIi be a contractive homeomorphism such that

    Li(x0)=xi1,Li(xN)=xi|Li(x)Li(x)|l|xx|  x,xI, (2.6)

    for some 0l<1. We consider N continuous mappings Fi:I×KK satisfying

    Fi(x0,y0)=yi1,Fi(xN,yN)=yi (2.7)

    We assume also that Fi is a Matkowski contraction with respect to the second variable, i.e., there exists function φi:[0,+)[0,+) satisfying the condition of item (2) of Definition 1 such that

    |Fi(x,y)Fi(x,y)|φi(|yy|),xI,y,yK. (2.8)

    In particular, we may consider the following system,

    {Li(x)=aix+kiFi(x,y)=g(y)+qi(x),

    where the real constants ai and ki and the function Fi are determined by conditions (2.6) and (2.7). It is clear that if g(y)=y1+y then Fi is not a Banach contraction but it is a Matkowski contraction with respect to the second variable.

    We define also the function wi:I×KIi×K by

    wi(x,y)=(Li(x),Fi(x,y)), (2.9)

    for all iJ. Assume that limm+φm(t)=0, where φ=supiJφi. Using (2.8) and (2.9) we get a wide variety of systems for different approximations problems, giving more flexibility and applicability of the fractal interpolation method. In the following result we will prove the existence of the fractal interpolation function (FIF) corresponding to the IFS {I×[a,b], wi, i=1,2,,N}. This result generalizes, in particular [2, Theorem 1] and the result in [14] since we only assume that the function Fi are Matkowski contractions with respect to the second variable.

    Theorem 3. The IFS {I×[a,b], wi, i=1,2,,N} defined above admits a unique attractor G, which is the graph of a continuous function f:I[a,b] satisfying f(xi)=yi, for i=0,1,,N.

    Proof. Let G be any attractor of the IFS {I×[a,b],wi, iJ} and then we have

    G=Ni=1wi(G). (2.10)

    In fact, for each iJ, the mapping wi may not satisfy the Matkowski contraction. But, if so, we may prove the existence and the uniqueness of the attractor G using the Hutchinson operator W defined in (1.1) (Theorem 2). In the following we will give the proof of Theorem 3. First, remark that the set ˜I={xI,y[a,b] with (x,y)G}, the projection of G into I, is equal to I. Indeed, since G=Ni=1wi(G), we can deduce that ˜I=Ni=1Li(˜I) and on the other hand the IFS {I,Li iJ} is hyperbolic having unique attractor I. Now, we present the proof of our result in two steps. We will prove that G is the graph of a function f defined on I and as a consequence we obtain the uniqueness of the attractor G since the union of two attractors is an attractor. In the second step we prove that f is continuous by studying the fixed point of Read-Bajraktarevíc operator.

    Step 1 :

    Let's prove that G is the graph of a function f:I[a,b] by proving that only one y-value corresponds to each x-value. First, remark that the IFS {I,Li iJ} is hyperbolic having unique attractor I=[x0,xN]. Therefore, using Eq (2.10), we obtain that for every xI there exists y[a,b] such that (x,y)G. In the following, we will prove that y is unique. For this, we consider, for i=0,,N, the set

    Xi={(x,y)G | x=xi}.

    case x=x0. Since for all i1, we have wi(X0)X0=, w1(X0)=X0. Moreover,

    d(w1(x0,y),w1(x0,y))=|F1(x0,y)F1(x0,y)|φ(d((x0,y),(x0,y))).

    Whence w1 has a unique fixed point on the compact metric space X0. In addition, using Theorem 2, the IFS {X0,w1} has a unique attractor X0 and then X0={(x0,y0)} as required.

    case x{x1,,xN}. Similarly, we have XN={(xN,yN)} and, for i=1,2,,N1, remark that Xi=wi+1(X0)wi(XN)={(xi,yi)}.

    case x{x0,,xN}. We will prove that, if there exist yx,yx[a,b] such that (x,yx), (x,yx)G then |yxyx|=0. Since G is compact, there exist i{1,2,,N} and ξIi such that

    supxI|yxyx|=|yξyξ|.

    Moreover, by the last two steps, we may assume that ξ(xi1,xi). Now, we may take t,t[a,b] such that wi(u)=(ξ,yξ) and wi(v)=(ξ,yξ) where u=(L1i(ξ),t)G and v=(L1i(ξ),t)G. It follows that

    yξ=Fi(L1i(ξ),t)andyξ=Fi(L1i(ξ),t).

    Therefore

    |yξyξ|=|Fi(L1i(ξ),t)Fi(L1i(ξ),t|φ(|tt|)φ(|yξyξ|).

    It follows, since φn(t)0 and then φ(t)t for t>0, that yξ=yξ.

    Step 2:

    We will prove that f is continuous. We consider the complete metric space (G,ρ) such that

    G={g:I[a,b)continuous such that g(x0)=y0 and g(xN)=yN}

    and the metric ρ is defined by

    ρ(g,h)=gh=max{|g(x)h(x)|,xI}.

    Now, we define the Read-Bajraktarevíc operator T on G by

    (T(g))(x)=Fi(L1i(x),gL1i(x)), xIi,iJ.

    Assume that we have shown that, f,gG, we have

    ρ(T(f),T(g))φ(ρ(f,g)) (2.11)

    then T has a unique fixed point ˜gG. Therefore the graph of ˜g is an attractor of the IFS {I×[a,b],wi,i=1,2,,N} which implies that ˜g=f and then f is continuous.

    Now, we will prove (2.11). Let f,gG and iJ. For any xIi, we have

    |Fi(L1i(x),f(L1i(x)))Fi(L1i(x),g(L1i(x)))|φ(|f(L1i(x))g(L1i(x))|)φ(ρ(f,g))).

    Now, observe that

    ρ(T(f),T(g))=supxIiiJ|Fi(L1i(x),f(L1i(x)))Fi(L1i(x),g(L1i(x)))|.

    Then, since I is compact, we get (2.11) and then T has a unique fixed point as required.

    In the following example we study the affect of box dimension when we consider a nonlinear IFS.

    Example 2. The box dimension is widely used to describe the complexity of certain figures and proved to be appropriate and effective method for fractal dimension estimate. The theoretical box dimension D is given by

    D=limϵ0logNϵlog(1/ϵ),

    where Nϵ is the minimum number of ϵ×ϵ squares needed to cover the graph of f. In this example, we consider, the data set Δ:={(0,0),(1/3,1),(2/3,1),(1,0)} and we define

    {L1(x)=13xL2(x)=13+13xL3(x)=23+13x{F1(x,y)=g1(y)+xF2(x,y)=g2(y)2x+1F3(x,y)=g3(y)1+x. (2.12)

    In Figure 1, we consider the case when the function gn are defined by gn(y)=αny with free parameters αn obeying αn(1,1), n=1,2,3. It is obvious that the system (2.12) satisfies (2.6), (2.7) and (2.8). The parameters αn are called vertical scaling factors and have important consequences on the box dimension D of the graph of the FIF, which will be denoted by fα, with α(0,1)3. Indeed, since we consider equally spaced interpolation points that do not all lie on the same line, we have [31]

    D:=1+log(3n=1|αn|)log(3) (2.13)
    Figure 1.  The graphs of fα's obtained from (2.12) with different αn and their corresponding box dimension D.

    when 3n=1|αn|>1. For different values of αn, we determine the box dimension of the corresponding FIF in Figure 1. In particular, we obtain smooth or non-smooth fractal interpolation function depending on the choice of scaling factors. Moreover, since for each n the function Fn is a Banach contraction with respect to the second variable, we assert that is a special case of FIF introduced in [2].

    In Figure 2, we consider again the system (2.12) but with different function g. From empirical evidence, we obtain that the function g has a great impact on the box dimension. It is natural to ask whether the box dimension of FIF depends on g in general. This seems to be wrong as we can see in Figure 2. Indeed, we obtain different values of the box dimension D that behaves non monotonically regardless of the fact that the norms of the functions used in the system are proportional.

    Figure 2.  The graphs of the FIF obtained from (2.12) with g(y)=34y1+34y2, g(y)=1334y1+34y2 and g(y)=1534y1+34y2 respectively.

    Let Δ:x0<x1<<xN be a partition of the real compact interval I=[x0,xN] and consider the data set {(xi,yi)I×Ri=0,1,,N}. Let K be a suitable compact subset of R containing yi, iJ0={0,,N}. Let fC(I,K), the normed space of real-valued continuous functions on I with values belonging to K. Assuming that C(I,K) is endowed with the uniform norm, we study, in this section, a new class of fractal interpolation functions which converge to f. Therefore, let, for nN, bn:C(I,K)C(I,K) be bounded and nonidentity linear operator such that, for every hC(I,K), we have

    bn(h)(x0)=h(x0),bn(h)(xN)=h(xN)andbn(h)h0asn. (3.1)

    Let gi, iJ, be a differentiable function with domain D. We assume that KD and supK|gi|<1 for all iJ. Now, let fC(I,K) that interpolates the data {(xi,yi),iJ0} and consider, for each nN, the IFS defined through the maps

    {Li(x)=aix+ki,Fn,i(x,y)=gi(y)+f(Li(x))gbn(f)(x),iJ (3.2)

    where the real constants ai and ki are determined by condition (2.6) and assume that (2.7) is satisfied. We may consider the case where gi(y):=gβ(y)=y1+βy, for β>0 and y>0. In this case, we have |Fn,i(x,y)Fn,i(x,y)|/|yy|=1/((1+βy)(1+βy)) for yy, and then the ratio |Fn,i(x,y)Fn,i(x,y)|/|yy| for yy can be made arbitrarily close to 1 by taking y and y sufficiently close to 0 and then Fn,i is not a Banach contraction with respect to the second variable. Nevertheless, we can prove that Fn,i is a Matkowski contraction. Therefore, for each β>0 and nN the IFS defined by (3.2) admits a unique attractor Gβ,n which is the graph of a continuous function fβn satisfying fβn(xi)=yi, for each iJ0. The FIF fβn is referred to as β-fractal function for f.

    The most widely studied bn(f) in the literature is the Bernstein polynomial of f defined by

    Bn(f,x)=1(xNx0)nnk=0(nk)(xx0)k(xNx)nkf(x0+k(xNx0)n)

    for all xI and nN. One can verify that Bn(f,x0)=h(x0) and Bn(f,xN)=f(xN). In addition, from classical approximation theory [32] we have that

    fBn(f,)32ωf(n1/2). (3.3)

    where ωf is the modulo of continuity of f defined as

    ωf(δ)=sup|xx|<δ|f(x)f(x)|.

    Since f is uniformly continuous on I, we obtain that ωf(n1/2)0 as n. When the IFS is defined using the Bernstein polynomial Bn(f,) and the function gβ, the fractal interpolation function fβn is called Bersntein β-fractal function of order n of f.

    Example 3. Let interpolation points {(0,1/5),(1/3,1/2),(1/2,1/3),(4/5,4/5),(1,3/5)} be given. We consider the functions gi(y)=y1+βiy and bn(f) is the Bernstein polynomial Bn(f,), where f is the piecewise linear function passing through the interpolation points given above.

    1) Let us consider a constant scaling vector β=(0.6,,0.6). Then the graph of the β-FIF for f generated by IFS (3.2), is plotted in Figure 3(a).

    Figure 3.  Graphs of the FIFs constructed from different vectors β.

    2) Take a non constant scaling vector β={β1,β2,β3,β4} then the graph of the β-FIF with the above variable parameters is displayed in Figure 3(b), (c).

    From Figure 3, we can notice that the self-similarity of the fractal interpolation curve shown in Figure 3(b), (c) is weaker than that of FIF in Figure 3(a). Hence, we can say that the FIFs with non constant scaling vector may have more flexibility and applicability. In fact, the FIFs generated by those IFSs with constant parameters usually have obvious self-similarity character, which could lead to the loss of flexibility, and might cause obvious errors in fitting and approximation of some complicated curves and non-stationary data that show less self-similarity.

    Our first main result in this section is the following.

    Theorem 4. Let ψC(I,K) be a function providing the data {(xi,yi),iJ0} and let fC(I,K) interpolate ψ with respect to these data. Let h:=maxi(xi+1xi) and assume, for some r>0, that

    ψf=O(hr).

    Then, the sequence {ˆfn}n of fractal interpolation functions, defined through the system (3.2), converges to ψ as h0 and n.

    Proof. We consider the complete metric space (G,ρ) where

    G={h:IKcontinuous such that h(x0)=y0 and h(xN)=yN}

    and ρ is the uniform metric on G. Now, for each nN, we define the Read-Bajraktarevíc operator Tn:GG by

    Tn(h)(x)=Fn,i(L1i(x),hL1i(x)),xIi,iJ.

    In addition, for all iJ, xIi and h1,h2G, we have

    |Fn,i(L1i(x),h1(L1i(x)))Fn,i(L1i(x),h2(L1i(x)))|φi(|h1(L1i(x))h2(L1i(x))|)φi(h1h2).

    Now observe that

    Tn(h1)Tn(h2)=supxIiiJ|Fn,i(L1i(x),h1(L1i(x)))Fn,i(L1i(x),h2(L1i(x)))|

    which implies that

    Tn(h1)Tn(h2)φi(h1h2),

    where φ=supiφi. Therefore, for nN, Tn is also a Matkowski contraction on the complete metric space (G,ρ) and therefore Tn possesses a unique fixed point ˆfn on G. It follows that ˆfn satisfies the following functional equation

    ˆfn(x)=gi(ˆfnL1i)(x)+f(x)gibn(f)(L1i(x)) (3.4)

    and then,

    ˆfnfgiˆfngif+gibn(f)gifγ[ˆfnf+bn(f)f],

    where γ=supK|gi|<1. As a consequence, we obtain

    ˆfnfγ1γbn(f)f. (3.5)

    Example 4. In this example, we consider the operator bn(f) to be the Bernstein polynomial of f. First notice that, from (3.3) and (3.5), the Bersntein β-fractal function of order n of f satisfies

    fβnf3γβ2(1γβ)ωf(n1/2).

    The most widely studied of fractal interpolation function has been obtained using the IFS

    Li(x)=aix+kiandFi(x,y)=αiy+qi(x),

    where the real constants ai and ki are determined by the condition (2.6), the functions qi are continuous satisfying conditions (2.7) and (2.8) and αi are free parameters such that αi(1,1). Therefore, the corresponding FIF will be indexed by α(1,1)N and will be denoted by fα named α-fractal interpolation function ([2,33]). As an application of Therorem 3.1, we can construct a fractal interpolation function ˆf, where (2.8) may be violated, and ˆf is as close as we want to fα. In addition, we have the following consequence.

    Corollary 1. Let α(0,1)N be a scaling vector and fα be a α-FIF interpolating data {(xi,yi),iJ0}. For every ϵ>0, there exist two approximating sequences {ln}n and {hn}n of fractal functions such that

    hn(x)fα(x)ln(x)andlnhnϵ.

    for all xI and nN0N.

    Proof. Theorem 4 ensures the existence of a sequence {ˆfn}n of fractal interpolation functions such that

    ˆfnfα<ϵ2,nN1N.

    Now define the fractal functions

    ln(x)=ˆfn(x)+ϵ2andhn(x)=ˆfn(x)ϵ2

    for all xI. It follows that

    ln(x)fαn+ϵ2ˆfnfαnfαn(x).

    Similarly, we have

    hn(x)fαnϵ2+ˆfnfαnfαn(x).

    1) Let {(xi,yj,zi,j),i=0,1,,N,j=0,1,,M}I×J×KR3 be a given data set. We denote Ii,Jj,Di,j and D by [xi1,xi],[yj1,yj],Ii×Jj and I×J respectively. We define mappings wi,j:D×KDi,j×K by

    wi,j(x,y,z)=(Li,j(x,y),Fi,j(x,y,z))

    where Li,j:DDi,j are contractive homeomorphisms and Fi,j:D×KK are Matkowski contractions. We strongly believe that the framework established in Section 3 remains true if we consider the GIFS

    {I×J×K,wi,j,i=1,,N,j=1,,M}.

    We find in this case that it is possible to construct a function f:I×JR whose graph is the attractor of a GIFS and interpolates the given data set. Such a result would be analogous to Theorem 2 of [34]. The pursuit of this question is encouraged by the application of fractal surfaces in many areas such as earth sciences, surface physics, and medical sciences [35,36,37,38,39].

    2) Let (Y,d) be a complete metric space and consider X=Y×Y. Recall the IFS {X,fn,n=1,,N} defined in Section 2 which admits a unique attractor GH(X). It is interesting to ask if the projection G onto Y itself is an attractor of an IFS. We conject that the projection is the graph of a continuous function which is not self-similar in general.

    3) Let Ω be a nonempty set and let ζ:Ω×Ω[1,+[ be a function. We define dζ:Ω×Ω[0,+[ such that, for all x,y,zΩ, we have

    (a) dζ(x,y)=0x=y;

    (b) dζ(x,y)=dζ(y,x);

    (c) dζ(x,y)ζ(x,y)[dζ(x,z)+dζ(z,y)].

    Then, (Ω,dζ) is called a ζ-metric space [40] which extends the b-metric space (ζ(x,y)=b) and the metric space (ζ(x,y)=1). We conject that the results in Section 2 remain true when we consider X to be a ζ-metric space and extends in particular [42, Theorem 3.7]. This requires, the introduction of new contractive conditions of general integral type in the setting of ζ-metric spaces and the definition of a generalization of the Hausdorff distance dζ on H(X).

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The authors extend their appreciation to the Deanship of Scientific Research at King Khalid University for funding this work through the Small Groups Project under grant number R.G.P.1/138/44.

    The authors declare there is no conflicts of interest.



    [1] M. F. Barnsley, Fractals Everywhere, 2nd edition, Academic Press, 1988.
    [2] M. F. Barnsley, Fractal functions and interpolation, Constr. Approx, 2 (1986), 303–329. https://doi.org/10.1007/BF01893434 doi: 10.1007/BF01893434
    [3] J. E. Hutchinson, Fractals and self-similarity, Indiana Univ. Math. J., 30 (1981), 713–747.
    [4] M. F. Barnsley, A. N. Harrington The Calculus of fractal interpolation functions, J. Approx. Theory, 57 (1989), 14–34. https://doi.org/10.1016/0021-9045(89)90080-4 doi: 10.1016/0021-9045(89)90080-4
    [5] N. A. Secelean, Countable iterated function systems, Far East J. Dyn. Syst., 3 (2001), 149–167.
    [6] K. Leśniak, Infinite iterated function systems: A multivalued approach, Bull. Pol. Acad. Sci. Math., 52 (2004), 1–8.
    [7] A. Mihail, R. Miculescu, Generalized IFSs on non-compact spaces, Fixed Point Theory Appl., 2010 (2010), 584215. https://doi.org/10.1155/2010/584215 doi: 10.1155/2010/584215
    [8] F. Strobin, J. Swaczyna, On a certain generalization of the iterated function system, Bull. Aust. Math. Soc., 87 (2013), 37–54. https://doi.org/10.1017/S0004972712000500 doi: 10.1017/S0004972712000500
    [9] K. R. Wicks, Fractals and Hyperspaces, Springer-Verlag, Berlin, 2006.
    [10] A. K. B. Chand, G. P. Kapoor, Generalized cubic spline fractal interpolation functions, SIAM J. Numer. Anal., 44 (2006), 655–676. https://doi.org/10.1137/0406110 doi: 10.1137/0406110
    [11] Y. Chen, G. A. Kopp, D. Surry, Interpolation of wind-induced pressure time series with an artificial network, J. Wind Eng. Ind. Aerodyn, 90 (2002), 589–615. https://doi.org/10.1016/S0167-6105(02)00155-1 doi: 10.1016/S0167-6105(02)00155-1
    [12] N. Vijender, Bernstein fractal trigonometric approximation, Acta Appl. Math., 159 (2018), 11–27. https://doi.org/10.1007/s10440-018-0182-1 doi: 10.1007/s10440-018-0182-1
    [13] P. Viswanathan, A. K. B. Chand, M. A. Navascuès, Fractal perturbation preserving fundamental shapes: Bounds on the scale factors, J. Math. Anal. Appl., 419 (2014), 804–817. https://doi.org/10.1016/j.jmaa.2014.05.019 doi: 10.1016/j.jmaa.2014.05.019
    [14] S. Ri, A new nonlinear fractal interpolation function, Fractals, 25 (2017). https://doi.org/10.1142/S0218348X17500633 doi: 10.1142/S0218348X17500633
    [15] S. Ri, New types of fractal interpolation surfaces, Chaos Solitons Fractals, 119 (2019), 291–297.
    [16] M. A. Navascués, C. Pacurar, V. Drakopoulos, Scale-free fractal interpolation, Fractal Fract, 6 (2022), 602. https://doi.org/10.3390/fractalfract6100602 doi: 10.3390/fractalfract6100602
    [17] J. Kim, H. Kim, H. Mun, Nonlinear fractal interpolation curves with function vertical scaling factors, Indian J. Pure Appl. Math., 51 (2020), 483–499. https://doi.org/10.1007/s13226-020-0412-x doi: 10.1007/s13226-020-0412-x
    [18] N. Attia, H. Jebali, Fractal interpolation functions with contraction condition of integral type, Chaos Solitons Fractal.
    [19] J. Matkowski, Integrable Solutions of Functional Equations, Instytut Matematyczny Polskiej Akademi Nauk(Warszawa), 1975.
    [20] S. Banach, Sur les opérations dans les ensembles abstraits et leur applications aux équations intégrales, Fund. Math., 3 (1922), 133–181.
    [21] A. Mihail, R. Miculescu, Applications of fixed point theorems in the theory of generalized IFS, Fixed Point Theory Appl., (2008), 312876. https://doi.org/10.1155/2008/312876 doi: 10.1155/2008/312876
    [22] N. Secelean, Generalized iterated function systems on the space l(X), J. Math. Anal. Appl., 410 (2014), 847–858. https://doi.org/10.1016/j.jmaa.2013.09.007 doi: 10.1016/j.jmaa.2013.09.007
    [23] F. Strobin, J. Swaczyna, A code space for a generalized IFS, Fixed Point Theory, preprint, arXiv: 1310.3097v2. https://doi.org/10.48550/arXiv.1310.3097
    [24] F. Strobin, Attractors of generalized IFSs that are not attractors of IFSs, J. Math. Anal. Appl., 422 (2015), 99–108. https://doi.org/10.1016/j.jmaa.2014.08.029 doi: 10.1016/j.jmaa.2014.08.029
    [25] R. Pasupathi, A. K. B. Chand, M. A. Navascuès, M. V. Sebastian, Cyclic generalized iterated function systems, Comput. Math. Methods, 3 (2021). https://doi.org/10.1002/cmm4.1202 doi: 10.1002/cmm4.1202
    [26] J. Jachymski, I. Jóź wik, Nonlinear contractive conditions: A comparison and related problems, Banach Center Publ. Polish Acad. Sci., 77 (2007), 123–146. https://doi.org/10.4064/bc77-0-10 doi: 10.4064/bc77-0-10
    [27] P. Viswanathan, A. K. B. Chand, M. A. Navascués, Fractal perturbation preserving fundamental shapes: Bounds on the scale factors, J. Math. Anal. Appl., 419 (2014), 804–817. https://doi.org/10.1016/j.jmaa.2014.05.019 doi: 10.1016/j.jmaa.2014.05.019
    [28] M. A. Navascués, Non-smooth polynomials, Int. J. Math. Anal., 1 (2007), 159–174.
    [29] E. Rakotch, A note on contractive mappings, Proc. Amer. Math. Soc., 13 (1962), 459–465. http://dx.doi.org/10.1090/S0002-9939-1962-0148046-1 doi: 10.1090/S0002-9939-1962-0148046-1
    [30] F. E. Browder, On the convergence of successive approximations for nonlinear functional equations, Nederl. Akad. Wetensch. Proc. Ser. Indag. Math., 71 (1968), 27–35. https://doi.org/10.1016/S1385-7258(68)50004-0 doi: 10.1016/S1385-7258(68)50004-0
    [31] M. F. Barnsley, J. Elton, D. P. Hardin, P. R. Massopust, Hidden variable fractal interpolation functions, SIAM J. Math. Anal., 20 (1989), 1218–1242. https://doi.org/10.1137/0520080 doi: 10.1137/0520080
    [32] S. G. Gal, Shape Preserving Approximation by Real and Complex Polynomials, Springer Science Business Media, 2010.
    [33] M. A. Navascuès, Fractal polynomial interpolation, Z. Anal. Anwend., 24 (2005), 401–418. https://doi.org/10.4171/ZAA/1248 doi: 10.4171/ZAA/1248
    [34] P. R. Massopust, Fractal surfaces, J. Math. Anal. Appl., 151 (1990), 275–290. https://doi.org/10.1016/0022-247X(90)90257-G doi: 10.1016/0022-247X(90)90257-G
    [35] P. Wong, J. Howard, J. Lin, Surfaces roughening and the fractal nature of rocks, Phys. Rev. Lett., 57 (1986), 637–640. https://doi.org/10.1103/PhysRevLett.57.637 doi: 10.1103/PhysRevLett.57.637
    [36] B. B. Nakos, C. Mitsakaki, On the fractal character of rock surfaces, Int. J. Rock Mech. Min. Sci. Geomech. Abstr., 28 (1991), 527–533. https://doi.org/10.1016/0148-9062(91)91129-F doi: 10.1016/0148-9062(91)91129-F
    [37] C. S. Pande, L. R. Richards, S. Smith, Fractal charcteristics of fractured surfaces, J. Met. Sci. Lett., 6 (1987), 295–297. https://doi.org/10.1007/BF01729330 doi: 10.1007/BF01729330
    [38] H. Xie, J. Wang, E. Stein, Direct fractal measurement and multifractal properties of fracture surfaces, Phys. Lett. A, 242 (1998), 41–50. https://doi.org/10.1016/S0375-9601(98)00098-X doi: 10.1016/S0375-9601(98)00098-X
    [39] X. C. Jin, S. H. Ong, Jayasooriah, Fractal characterization of Kidney tissue sections, IEEE Int. Conf. Eng. Med. Biol. Baltimore, 2 (1994), 1136–1137. https://doi.org/10.1109/IEMBS.1994.415361 doi: 10.1109/IEMBS.1994.415361
    [40] M. Samreen, T. Kamran, M. Postolache, Extended b- Metric space, extended b-comparison function and nonlinear contractions, U.P.B. Sci. Bull., Series A, 80 (2018).
    [41] C. Wolf, A mathematical model for the propagation of a hantavirus in structured populations, Discrete Contin. Dyn. Syst. B, 4 (2004), 1065–1089. https://doi.org/10.3934/dcdsb.2004.4.1065 doi: 10.3934/dcdsb.2004.4.1065
    [42] S. S. Al-Bundi, Iterated function system in -Metric spaces, Bol. Soc. Paran. Mat., 40 (2022), 1–10. https://doi.org/10.5269/bspm.52556 doi: 10.5269/bspm.52556
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