Abstract
Constructions of the (global) fractal interpolation functions on standard function spaces got a lot of attention in the last centuries. Motivated by the newly introduced local fractal functions corresponding to a local iterated functions system which is the generalization of the traditional iterated functions system we construct the local non-affine \(\alpha \)- fractal functions in this article. A few examples of the graphs of these functions are provided. A fractal operator which takes the classical function to its local fractal counterpart is defined and some of its properties are also studied.
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1 Introduction
Fractal functions are used as an alternative tool for interpolation and approximation purposes. It was first introduced by Barnsley [1] such that the graph of this function is the attractor of some iterated function system (IFS). Fractal functions usually are non-smooth functions and they interpolate a set of given data, for example, \(\{\, (x_i,y_i) \in {\mathbb {R}}^2~:~x_i<x_{i+1},~i=1,~2,~\dots ,~K \, \}\), which is quite different from the traditional interpolation techniques, where one can only produce piece-wise differentiable interpolation functions. Fractal interpolation functions are used in many diverse areas, like data analysis, image compression, signal processing etc [17,18,19,20,21]. For instance, in [19] Fractal functions are used to predict the seven-day moving average of daily positive cases due to COVID-19, for the upcoming three months from December 13, 2021, of six countries including India.
Motivated by the work of Barnsley [1], Navascués [3] defined a special kind of fractal function known as \(\alpha \)-fractal function. These functions not only interpolate but also approximate any continuous function defined on compact intervals of \({\mathbb {R}}\). By choosing the base function (see Sect. 2.3) as a nowhere differentiable function ( like, a Weierstrass function [16]) one can have non-smooth analogues of a continuous function. In consecutive papers [9,10,11,12,13,14], fractal dimension of \(\alpha \)-fractal function is also studied.
In a more general and flexible setting Masssopust [6] defined local fractal functions, which are fixed points of a particular class of Read-Bajactarević (RB) operators defined on the space of all bounded functions. The author also showed that the graphs of these local fractal functions are attractors of a specific local IFS. Massopust also defined local fractal functions on unbounded domains and derived conditions so that local fractal functions are elements of various standard function spaces like Lebesgue spaces, the smoothness spaces, the homogeneous Hölder spaces, the Sobolev spaces, Besov and Triebel-Lizorkin spaces (see [6,7,8]).
In this paper, we construct a generalised version of \(\alpha \)-fractal functions through the lens of local fractal functions. These local \(\alpha \)-fractal functions interpolate as well as approximate bounded functions on compact intervals of \({\mathbb {R}}\).
This paper is structured as the following. In Sect. 2 first, we introduce iterated function systems and define the attractor of an IFS, then we provide the construction of fractal interpolation functions and \(\alpha \)-fractal functions, also a brief summary of local fractal functions is given. In Sect. 3, we give the construction of the local \(\alpha \)-fractal function, provide some examples and also define an operator attached to local \(\alpha \)-fractal functions and study some properties of this operator.
2 Preliminaries
2.1 Iterated function system
Let X be a topological space and \(\beta _i:X \rightarrow X\) \((i=1,2,\dots ,K; K\in {\mathbb {N}})\) are continuous functions. The space X with the functions \(\beta _i\) is called an iterated function system or IFS and it is denoted by \(\{\, X;\beta _i:i=1,2,\dots ,K \, \}\). Let \(H_X\) be the set of all non-empty compact subsets of X. Define the Hutchinson operator \(Q:H_X \rightarrow H_X\) by
\(S \in H_X\). When X is a metric space with metric \(d_X\), we can define a metric \(d_H\) on the space \(H_X\) by,
for \(S_1,S_2 \in H_X\), where
When \((X,d_X)\) is complete then \((H_X,d_H)\) is also complete. The IFS \(\{\, X;\beta _i:i=1,2,\dots ,K \, \}\) is called hyperbolic if the maps \(\beta _i\)’s are contractions, that is, there exists \(\theta _i \in [0,1)\) such that
And in that case, Q is also a contraction map on the complete metric space \((H_X,d_H)\) [15]. A set \(B\in H_X\) is called an attractor of the IFS \(\{\, X;\beta _i:i=1,2,\dots ,K \, \}\), if
When Q is a contraction on the complete metric space \((H_X,d_H)\) by the Banach fixed point theorem there exists a unique set \(B \in H_X\) such that \(Q(B)=B\) i.e. B is the unique attractor of the associated IFS \(\{\, X;\beta _i:i=1,2,\dots , K \, \}\).
2.2 Fractal interpolation function
Let \(\{\, x_i: i=0,1,\dots ,K \, \} \subset {\mathbb {R}}\), where \(K \in {\mathbb {N}}\), be such that \(x_{i} < x_{i+1},~ \forall i \in \{\, 0,1, \dots , K-1 \, \}.\) Let \(A=[x_0,x_K]\) be a closed and bounded interval. Let \(\{\, (x_i,y_i): i=0,1, \dots , K\, \}\) be a set of data points. Setting \(J_i=[x_{i-1},x_i]\), define \(L_i:A \rightarrow J_i\) be such that,
and
where \(l \in [0,1)\) and for all \(c,d \in A\) and \(i=1,2,\dots ,K\). Let \(\alpha _i \in (-1,1)\) and continuous maps \(F_i:A \times {\mathbb {R}} \rightarrow {\mathbb {R}}\) be such that
and
for all \(i=1,2,\dots ,K\) and \(c \in A\) and \(d_1,d_2 \in {\mathbb {R}}\). Define the maps \(w_i:A \times {\mathbb {R}} \rightarrow J_i \times {\mathbb {R}}\) by
Let \({\mathcal {G}}=\{ \, g: A \rightarrow {\mathbb {R}} \mid g~\text {is continuous and}~g(x_0)=y_0,~g(x_N)=y_N \, \} .\) \({\mathcal {G}}\) forms a complete metric space with respect to the sup metric
\(d_\infty (g_1,g_2)=\sup \{\, \vert {g_1(x)-g_2(x)} \vert :~x\in A \, \}\).
Theorem 1
[Barnsley [1]] The IFS \( \left\{ \, A\times {\mathbb {R}};w_i:i=1,2,\dots ,K \, \right\} \) has a unique attractor G, which is the graph of a continuous function \({\hat{f}}:A \rightarrow {\mathbb {R}}\) such that \({\hat{f}}(x_i)=y_i,~~ i=0,1,\dots ,K\).
Following is an example of a fractal interpolation function.
Example 1
Let \(\{(i,\sin {(6*i)}) \mid i=0,1/2,1\}\) be a data set. A FIF corresponding to this data set is given in Fig. 1.
Define an operator \(T: {\mathcal {G}} \rightarrow {\mathcal {G}}\) by,
Then T is a contraction on \({\mathcal {G}}\), i.e for \(g_1,g_2 \in {\mathcal {G}}\)
where \(\vert {\alpha } \vert _\infty :=\max \{\, \vert {\alpha _i} \vert :i=1,2,\dots ,K \, \}\). Since \(\alpha _i \in (-1,1)\), \(\vert {\alpha } \vert _\infty \in [0,1)\).
Again by Banach fixed point theorem, T being a contraction on the complete metric space \({\mathcal {G}}\), has a unique fixed point which is \({\hat{f}}\) itself, i.e. \(T({\hat{f}})={\hat{f}}\). \({\hat{f}}\) is called a FIF corresponding to the data set \(\{\, (x_i,y_i):i=0,1,\dots ,K \, \}\).
One of the widely popular ways of defining a FIF is by choosing the maps \(L_i\)’s and \(F_i\)’s as the following,
where the constants \(a_i,~d_i\) are determined by (6) and the maps \(q_i:A \rightarrow {\mathbb {R}}\) are chosen continuous functions such that (8) holds. If we choose \(q_i(x)\) to be linear then the corresponding FIF is called an Affine FIF (cf. [1, 2]).
2.3 Construction of \(\alpha \)-fractal function
Set \({\mathcal {C}}(A)\) as the space of all real valued continuous functions on A equipped with the sup norm \(\Vert {g} \Vert _\infty =\sup \{\, \vert {g(x)} \vert :x \in A \, \}\). Let \(g \in {\mathcal {C}}(A)\). Navascués in [3, 4] took
where \(b \in {\mathcal {C}}(A)\) with \(b(x_0)=f(x_0), ~b(x_K)=f(x_K)\) and \(b \ne g\). b is known as the base function.
Definition 1
[4] Let \(g^\alpha \) be the continuous function whose graph is the attractor of the IFS (10), (13) and (14). Then, the function \(g^\alpha \) is called the \(\alpha \)-fractal function associated to g with respect to the base function b(x) and the partition \(\Delta =(x_0<x_1<\dots <x_K)\).
Following is an example of a \(\alpha \)-fractal function.
Example 2
The Fig. 2 represents a \(\alpha \)-fractal function corresponding to the function \(\sin {(6x)}\).
The choices made in (13) and (14), shapes T into a particular form as the following,
Hence \(g^\alpha \) satisfies the following self-referential equation
2.4 Construction of local fractal function
In this section, we introduce the construction, given by P. R. Massopust [6] of bounded local fractal functions. These functions are defined as the fixed points of a particular type of RB operators acting on the complete metric space of bounded functions.
For this purpose, let \(\{\, Y_i: i=1,~2,~\dots ,~K \, \}\) be a family of nonempty connected subsets of a connected topological space Y. Suppose \(\{\, \lambda _i: Y_i \rightarrow Y \mid i=1,~2,~\dots ,~K \, \}\) is a family of injective mappings with the property that \(\{\, \lambda _i(Y_i):~i=1,~2,~\dots ,~K \, \}\) forms a partition of Y. Now suppose that \((Z, d_Z)\) is a complete linear metric space and \(B(Y, Z):= \{\, g: Y \rightarrow Z \mid g~\text {is~bounded} \, \},\) endowed with the sup metric \(d(g_1,g_2)=\sup \{\, d_Y(g_1(y),g_2(y)):~y \in Y \, \}\).
For \(i \in \{\, 1,~2,~ \dots ,~ K \, \} \), define \(\gamma _i: Y_i \times Z \rightarrow Z \) be a mapping such that \(\exists ~ r \in [0,1) \) and \(\forall ~ y \in Y_i\) and \(\forall ~ z_1,z_2 \in Z\)
That is, \(\gamma _i\) is uniformly contractive in the second variable.
Now we can define a RB operator \(T: B(Y, Z) \rightarrow Z^Y\) by
where \(h_i:=h\mid _{Y_i}\) and
One can check that T is a well-defined contraction on the complete metric space B(Y, Z) and hence by the Banach Fixed Point Theorem T has, therefore, a unique fixed point \({g}\) in B(Y, Z). This unique fixed point is called a local fractal function \({g} = {g}_\Phi \) (generated by T) [6].
3 Local \(\alpha \)-fractal function
Let \(\{\, A_i: i=1,2, \dots , K \, \}\) be a collection of non-empty connected subsets of \(A=[x_0,x_K]\) such that \(x_0 \in A_i, \forall i \in \{\, 1,2, \dots ,K \, \}\) and \(x_K \in A_K.\)
Also let, \(\lambda _i: A_i \rightarrow A\) be injective maps with the following properties:
-
1.
\(\{\, \lambda _i(A_i): i=1,2, \dots ,K \, \}\) forms a partition of A, i.e.
-
\(\bigcup _{i=1}^N \lambda _i(A_i) = A\) and
-
\(\lambda _i(A_i) \bigcap \lambda _j(A_j) = \emptyset \).
-
-
2.
$$\begin{aligned} \lambda _i(x_0)=x_{i-1}, \forall i=1,2,\dots , K ~~\text {and} ~~\lambda _K(x_K)=x_K \end{aligned}$$(19)
For \(i \in \{\, 1,2, \dots , K \, \} \), define \(\gamma _i: A_i \times {\mathbb {R}} \rightarrow {\mathbb {R}} \) be a mapping for which \(\exists ~ r \in [0,1) \) such that, \(\forall ~ a \in A_i\) and \(\forall ~ b_1,b_2 \in {\mathbb {R}}\)
that is, \(\gamma _i\) is uniformly contractive in the second variable.
Set \(B(A,{\mathbb {R}})=\{\, g:A \rightarrow {\mathbb {R}} \mid g~\text {is bounded} \, \}\) and define a metric \(d_\infty (f,g)= \sup _{x \in A}~\vert {f(x)-g(x)} \vert \). Then \((B(A,{\mathbb {R}}),d_\infty )\) is a complete metric space.
Define a RB operator \(T: B(A, {\mathbb {R}}) \rightarrow {\mathbb {R}}^A \) by
where \(h \in B(A,{\mathbb {R}})\), \( \chi _S (x)= {\left\{ \begin{array}{ll} 1, &{} x \in S\\ 0, &{} x \notin S. \end{array}\right. }\) and \(h_i:= h \mid _{A_i}\).
Note that T is well-defined and \(T(B(A, {\mathbb {R}})) \subseteq B(A, {\mathbb {R}})\).
Also, for \(h,g \in B(A,{\mathbb {R}})\)
which shows that T is a contraction on the complete metric space \(B(A, {\mathbb {R}})\). Hence by Banach Fixed Point theorem there exists a unique \({h} \in B(A,{\mathbb {R}})\) such that \(T({h})={h}\), that is T has a unique fixed point \({h}\) in \(B(A,{\mathbb {R}})\). This unique fixed point is called local fractal function \({h}={h}_{{\textbf {T}}}\) (generated by T).
Next, we would like to a particular form of the maps \(\gamma _i\). Let the maps \(\gamma _i: A_i \times {\mathbb {R}} \rightarrow {\mathbb {R}}\) be defined by the following,
where \(q_i,\alpha _i \in B(A_i,{\mathbb {R}}),~i \in \{1,2, \dots , K\}.\)
Now, for \(a \in A_i\) and \(b_1,b_2 \in {\mathbb {R}}\)
where \(\Vert {\alpha _i} \Vert _{\infty ,A_i}:=\sup \{\, \vert {\alpha _i(x)} \vert : x \in A_i \, \}\) and \(\vert {\alpha } \vert _\infty :=\max \{\, \vert {\alpha _i} \vert _{\infty ,A_i}:i=1,2,\dots ,K \, \}\). Hence for \(\gamma _i\) to satisfy (20) we need \(\vert {\alpha } \vert _\infty \in [0,1)\).
Continuing with this choice of \(\gamma _i\)’s, the operator T takes the following form
Hence by Theorem 3 in [6] there exist a unique \({h} \in B(A,{\mathbb {R}})\) such that \(T({h})={h}\) i.e \({h}\) satisfies the self-referential equation
where \({h}_i={h}\mid _{A_i}\).
This unique fixed point \({h}\) in (24) is called bounded local fractal function generated by T with respect to the set of functions \(\{\, q_i \mid i=1,2,\dots ,K \, \}\) and \(\{\, \alpha _i \mid i=1,2,\dots ,K \, \}\).
Let \({\mathcal {H}}:=\{\, g \in B(A,{\mathbb {R}}) \mid g(x_0)=y_0~~\text {and}~~g(x_K)=y_K \, \}\). Then \(({\mathcal {H}},d_\infty )\) is a complete metric space.
Now we would like to consider the functions \(q_i\) in a special form,
where \(g,b \in {\mathcal {H}}\) are such that \(g \ne b\) and \(g(x_i)=y_i\) for \(i=0,1,\dots ,K\).
By this choice, it is clear that \(q_i \in B(A_i, {\mathbb {R}})\) and hence the operator in (23) can be written in the following form,
or, equivalently
Again by using (26) and (19), for \(h \in {\mathcal {H}}\) we have
Similarly, it can be checked that \(Th(x_K)=y_K\).
So we can consider T as an operator on \({\mathcal {H}}\) i.e. \(T: {\mathcal {H}} \rightarrow {\mathcal {H}}\) is given by
Hence T is a contraction mapping on the complete metric space \(({\mathcal {H}},d_\infty )\). So T possesses a unique fixed point say \({g}^\alpha \in {\mathcal {H}}\).
Hence for fixed \(g,b \in {\mathcal {H}}\) and for a selected collection of non-empty connected subsets \({{\textbf {P}}}:=\{\, A_i \subseteq A: i=1,2, \dots ,K \, \}\) and injective maps \({{\textbf {F}}}:=\{\, \lambda _i:A_i \rightarrow A \mid i=1,2, \dots ,K \, \}\) there is a unique \({g}^\alpha \in {\mathcal {H}}\) such that \(T({g}^\alpha )={g}^\alpha \) i.e. \({g}^\alpha \) satisfies the self-referential equation
where\({g}_i^\alpha ={g}^\alpha \mid _{A_i}\).
\({g}^\alpha \) will be called the local \(\alpha \)-fractal function associated to g with respect to b and \({{\textbf {P}}}, {{\textbf {F}}}\).
Using (19) and since \({g}^\alpha \in {\mathcal {H}}\), \(b \in {\mathcal {H}}\) and \(g(x_i)=y_i,~\forall i \in \{\, 0,1,\dots ,K \, \}\), we have for \(i=0,1,\dots ,K-1\)
This shows that \({g}^\alpha \) interpolates g at \(\{\, x_i: i=0,1,\dots ,K \, \}\).
Remark 1
If for all \(i \in \{\, 1,2,\dots ,K \, \},~\alpha _i\equiv 0\) that is \(\vert {\alpha } \vert _\infty =0\), then (28) implies \({g}^\alpha =g\).
Theorem 2
Let \(\{\, (x_i,y_i) \in {\mathbb {R}} \times {\mathbb {R}}:~ x_i < x_{i+1},~i=0,~1,\dots ,~K\}\) be a data set. Let \({{\textbf {P}}}:=\{\, A_i \subseteq A: i=1,2, \dots ,~K \, \}\) be a collection of non-empty connected subsets and \({{\textbf {F}}}:=\{\, \lambda _i: ~A_i \rightarrow A \mid i=1,2, \dots ,~K \, \}\) be a collection of injective maps with properties mentioned above. Let \(g \in B(A,{\mathbb {R}})\) such that \(g(x_i)=y_i,~i=0,~1,\dots ,~K\) be fixed. Let
be such that \(\vert {\alpha } \vert _\infty \in [0,1)\). Also, let \(b\in {\mathcal {H}}\) with \(b\ne g\). Define \(T: {\mathcal {H}} \rightarrow {\mathcal {H}}\) by
where \(h_i:= h \mid _{A_i}\). Then T is a contraction on the complete metric space \({\mathcal {H}}\) and its unique fixed point \({g}^\alpha \) satisfies the self-referential equation
where \({g}_i^\alpha ={g}^\alpha \mid _{A_i}\). Also \({g}^\alpha \) interpolates g at \(\{\, x_i: i=0,1,\dots ,K \, \}\).
Proof
The proof follows from the previous analysis. \(\hfill\square \)
A Local \(\alpha \)-fractal function corresponding to a continuous function is given in the following example.
Example 3
Let the data set be \(\left\{ \, (\frac{i}{16},\sin {\frac{6\cdot i}{16}}):\right.\) \(\left.i=0,~1,\dots ,~16 \, \right\} \). Let \(A=[0,1].\) Let \(A_i=[0,\frac{i}{16}]\) and \(\lambda _i=\frac{x}{i}+\frac{i-1}{16},~~i=1,~2,\dots ,~16\). Fix \(g(x)=\sin {6x}\). Then by choosing \(b(x)=\sin {6}\cdot x\) the corresponding local \(\alpha \)-fractal function is shown in Fig. 3a and 3b with respect to the following scale vectors
-
1.
\(\alpha _i= {\left\{ \begin{array}{ll} 0.2, &{} i=odd\\ -0.2, &{} i=even; \end{array}\right. }\)
-
2.
\(\alpha _i(x)= {\left\{ \begin{array}{ll} 0.5\cdot \sin {60x}, &{} i=1,5,9,13\\ \exp {-2x-1} \cdot 0.5 \cdot \sin {60x}, &{} i=2,6,10,14\\ 0.5 \cdot \cos {30x}, &{} i=3,7,11,15\\ 0.5 \cdot \sin {40x}, &{} i=4,8,12,16 \end{array}\right. }\)
A Local \(\alpha \)-fractal function corresponding to a discontinuous function is given in the following example.
Example 4
Let the data set be \(\left\{ \, (\frac{i}{16},\lfloor \frac{10.5i}{16}\rfloor \right.\) \(\left.* \sin {\frac{6i}{16}}:~i=0,~1,\dots ,~16 \, \right\} \). Let \(A=[0,1].\) Let \(A_i=[0,\frac{i}{16}]\) and \(\lambda _i=\frac{x}{i}+\frac{i-1}{16},~~i=1,~2,\dots ,~16\). Fix \(g(x)=\lfloor 10.5x \rfloor * \sin {6x}\). Then by choosing \(b(x)=10\cdot \sin {6} *x\) and the corresponding local \(\alpha \)-fractal function is shown in figure 4a and 4b with respect to the following scale vectors
-
1.
\(\alpha _i= {\left\{ \begin{array}{ll} 0.2, &{} i=odd\\ -0.2, &{} i=even, \end{array}\right. }\)
-
2.
\(\alpha _i(x)= {\left\{ \begin{array}{ll} 0.5\cdot \sin {60x}, &{} i=1,5,9,13\\ \exp {-2x-1} \cdot 0.5 \cdot \sin {60x}, &{} i=2,6,10,14\\ 0.5 \cdot \cos {30x}, &{} i=3,7,11,15\\ 0.5 \cdot \sin {40x}, &{} i=4,8,12,16 \end{array}\right. }\)
Remark 2
As we can see in the above examples that the local \(\alpha \)-fractal functions are discontinuous in both cases. This is not always the case though, for example, one simple way of getting a continuous local \(\alpha \)-fractal function is by choosing \(K=1\) in the corresponding construction (see Sect. 3).
Again from (28) we have
which gives
since this is true for all \(i \in \{1,2,\dots ,K \} \) we can deduce that,
and hence
Let us define an operator \({\mathcal {L}}^\alpha : {\mathcal {H}} \rightarrow {\mathcal {H}}\) by \(g \hookrightarrow {g}^\alpha \), that is \({\mathcal {L}}^\alpha \) associates the local \(\alpha \)-fractal function \({g}^\alpha \) with g. Also, it is clear that \({\mathcal {L}}^\alpha ={\mathcal {L}}^\alpha _{b, {\textbf {P,F}}}\) depends on b and \({{\textbf {P}}}\), \({{\textbf {F}}}\).
Proposition 1
If b and \({{\textbf {P}}}\), \({{\textbf {F}}}\) are fixed then for all \(g,f \in {\mathcal {H}}\)
that is \({\mathcal {L}}^\alpha \) satisfies the Lipschitz condition on \({\mathcal {H}}\).
Proof
By the definition of \({\mathcal {L}}^\alpha \) and using (28), we have
which gives
Hence
which in turn implies that
Hence
\(\hfill\square \)
Theorem 3
The operator \({\mathcal {L}}^\alpha : {\mathcal {H}} \rightarrow {\mathcal {H}}\) is continuous on \({\mathcal {H}}\).
Proof
By proposition 1, we see that \({\mathcal {L}}^\alpha \) satisfies the Lipschitz condition on \({\mathcal {H}}\) and hence \({\mathcal {L}}^\alpha \) is continuous on \({\mathcal {H}}\). \(\hfill\square \)
Now, let us choose \(b=g \circ u\) where \(u \in B(A,A)\) and \(u(x_0)=x_0\), \(u(x_K)=x_K\), then the operator \({\mathcal {L}}^\alpha ={\mathcal {L}}^\alpha _{u, {\textbf {P,F}}}\), which assigns the local \(\alpha \)-fractal function \(g^\alpha \) to g is linear, as \(g,h \in {\mathcal {H}}\) implies
and for \(\lambda _1, \lambda _2 \in {\mathbb {R}}\), we have
\(\text {for}~ i=1,2, \dots , K.\)
Since the solution of the Eq. (28) is unique, for all \(\lambda _1, \lambda _2 \in {\mathbb {R}}\), we have
Again using \(b=g\circ u\) in Eq. (29), we have
and consequently, we can derive the following
which in turn implies
It follows that the operator \({\mathcal {L}}^\alpha \) is a linear and bounded operator.
Theorem 4
Fixing the base function \(b=g\circ u\), for \(u \in B(A,A)\) and \(u(x_0)=x_0\), \(u(x_K)=x_K\), the operator \({\mathcal {L}}^\alpha : {\mathcal {H}} \rightarrow {\mathcal {H}}\) becomes linear and bounded.
Proof
This statement follows from the above considerations. \(\hfill\square \)
4 Conclusion and future directions
In this paper, we constructed the local \(\alpha \)-fractal function on a closed interval [a, b]. We provided a couple of examples of the local \(\alpha \)-fractal functions corresponding to a continuous function as well as a discontinuous function. Then we studied some properties of the fractal operator which assigns a function with its corresponding local \(\alpha \)-fractal function. By modifying the underlying conditions suitably one can define local \(\alpha \)-fractal functions in Lebesgue spaces, Sobolev spaces and other standard function spaces. One also expects to define local \(\alpha \)-fractal functions for functions defined on non-compact unbounded domains of \({\mathbb {R}}\). One might also generalise this paper by considering the scale-free fractal interpolation (see [5]). As mentioned in the introduction, Fractal interpolation functions are used in data analysis to interpolate real-world data sets that can not be interpolated by traditional polynomial interpolants. As the data sets involved are often discontinuous, so the local \(\alpha \)-fractal functions might be more suitable to study this kind of data as compared to classical fractal interpolation functions.
Data Availability Statement
No data associated in the manuscript.
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AB acknowledges the Council of Scientific & Industrial Research (CSIR), India, for the financial support under the scheme “JRF” (FileNo. 08/0155(12963)/2022-EMR-I). Md.NA acknowledges the Department of Science and Technology (DST), Govt. of India, for the financial support under the scheme “Fund for Improvement of S &T Infrastructure (FIST)” (File No. SR/FST/MS-I/2019/41).
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Framework of Fractals in Data Analysis: Theory and Interpretation. Guest editors: Santo Banerjee, A. Gowrisankar.
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Banerjee, A., Akhtar, M.N. & Navascués, M.A. Local \(\alpha \)-fractal interpolation function. Eur. Phys. J. Spec. Top. 232, 1043–1050 (2023). https://doi.org/10.1140/epjs/s11734-023-00865-x
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DOI: https://doi.org/10.1140/epjs/s11734-023-00865-x