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The structure of fuzzy fractals generated by an orbital fuzzy iterated function system

  • Irina Savu EMAIL logo , Radu Miculescu and Alexandru Mihail
Published/Copyright: May 25, 2023
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Abstract

In this article, we present a structure result concerning fuzzy fractals generated by an orbital fuzzy iterated function system ( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) . Our result involves the following two main ingredients: (a) the fuzzy fractal associated with the canonical iterated fuzzy function system ( ( I N , d Λ ) , ( τ i ) i I , ( ρ i ) i I ) , where d Λ is Baire’s metric on the code space I N and τ i : I N I N is given by τ i ( ( ω 1 , ω 2 , ) ) ( i , ω 1 , ω 2 , ) for every ( ω 1 , ω 2 , ) I N and every i I ; (b) the canonical projections of certain iterated function systems associated with the fuzzy fractal under consideration.

MSC 2010: 28A80; 37C70; 54H20

1 Introduction

1.1 Generalities concerning iterated function systems, iterated fuzzy set systems and orbital fuzzy iterated function systems

Iterated function systems (which were initiated by Hutchinson in [1]) provide a standard framework for self-similarity. Some nice surveys on this theory are presented in [25]. Because of their attribute to squeeze large amount of data into a few number of parameters, they have nice applications in image processing via the so-called inverse problem, which asks to find an iterated function system whose attractor approximates a target set with a prescribed precision. In the case of image with gray levels the aforementioned theory involves a class of measures generated by adding a probability system to the iterated function system. An alternative approach, based on considering images as functions rather that measures, was introduced by Cabrelli and Molter [6] and Cabrelli et al. [7]. More precisely, they combined the idea of representation of a image as a fuzzy set with the Hutchinson’s theory and introduced the concept of iterated fuzzy set system (IFZS). In this way, they succeeded in generating images with gray levels as attractors of IFZSs, i.e., as the fixed point of corresponding fuzzy operators. In addition, they proved that one can find an IFZS whose attractor approximates a target set with a imposed precision. For some other results along this line of research, see [810].

The articles [1113] deal with the concept of orbital iterated function system, which is an iterated function system consisting of continuous functions satisfying Banach’s orbital condition. It is a real generalization of the idea of the iterated function system since its associated fractal operator is weak Picard, but it is not necessarily Picard. The fuzzification idea applied to the framework of orbital iterated function systems leads to the study of the orbital fuzzy iterated function system in [14], whose corresponding fuzzy operator is weak Picard. Its fixed points are called fuzzy fractals. In [15], we presented a structure result concerning fuzzy fractals associated with an orbital fuzzy iterated function system. We proved that such an object is perfectly determined by the action of the initial term of the Picard iteration sequence on the closure of the orbits of certain elements.

1.2 The results of this article

Given a fuzzy iterated function system S Z = ( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) , let us denote by u S its fuzzy fractal and by u Λ the fuzzy fractal of the canonical iterated fuzzy function system ( ( Λ ( I ) , d Λ ) , ( τ i ) i I , ( ρ i ) i I ) , where d Λ is Baire’s metric on the code space Λ ( I ) and τ i : Λ ( I ) Λ ( I ) is given by τ i ( ω ) = i ω for every ω Λ ( I ) and every i I .

First, we prove (Theorem 3.4) that u S = π ( u Λ ) , where π is the canonical projection associated with the iterated function system ( ( X , d ) , ( f i ) i I ) . In addition (Theorem 3.2), we prove that u Λ is perfectly determined by the admissible system of gray level maps ( ρ i ) i I .

Finally (Theorem 3.5), on the basis of the main result from [15] and the aforementioned results, we are able to provide a structure result concerning the fuzzy fractals generated by an orbital fuzzy iterated function system S Z . It involves u Λ and the canonical projections of certain iterated function systems associated with the fuzzy fractal under consideration.

2 Preliminaries

2.1 Some basic notations

For a function f : X X and n N = def { 1 , 2 , } , by f [ n ] , we designate the composition of f by itself n times.

Given a metric space ( X , d ) , a function f : X X is called weak Picard operator if there exists lim n f [ n ] ( x ) , and it is a fixed point of f for every x X . If a weak Picard operator has a unique fixed point, then it is called Picard operator.

Given a metric space ( X , d ) , by h we designate the Hausdorff-Pompeiu metric on X , i.e. the function h : P b , c l ( X ) × P b , c l ( X ) [ 0 , ) , described by

h ( K 1 , K 2 ) = max { sup x K 1 d ( x , K 2 ) , sup x K 2 d ( x , K 1 ) } ,

for every K 1 , K 2 P b , c l ( X ) = { A X A and A is bounded and closed } .

For a family of functions ( f i ) i I , where f i : X R , we shall use the following notation:

sup i I f i = not i I f i .

Lemma 2.1

Given a family ( a i j ) i I , j J of real numbers, where I is finite and J is infinite, we have

max i I max j J a i j = max j J max i I a i j ,

provided that

sup j J a i j = max j J a i j ,

for every i I .

Proof

For j J , we shall consider i j I such that

max i I a i j = a i j j .

On the one hand, we have

(1) max i I max j J a i j max j J max i I a i j .

Indeed,

a i j a i j j ,

for all i I and j J . Hence,

sup j J a i j sup j J a i j j ,

so

max j J a i j max j J a i j j = max j J max i I a i j ,

for all i I and the justification of (1) is completed.

On the other hand, we have

(2) max j J max i I a i j max i I max j J a i j .

Indeed,

a i j sup j J a i j = max j J a i j ,

for all i I and j J . Therefore,

max i I a i j max i I max j J a i j ,

i.e.,

a i j j max i I max j J a i j ,

for every j J . Hence,

sup j J a i j j = max j J a i j j = max j J max i I a i j max i I max j J a i j

and the justification of (2) is finished.

By taking into account (1) and (2), the proof is completed.□

2.2 Fuzzy sets

Let us consider the sets X and Y .

The elements of

{ u : X [ 0 , 1 ] } = not X

are called fuzzy subsets of X .

If there exists x X such that u ( x ) = 1 , then we say that u X is normal.

A nonzero function ρ : [ 0 , 1 ] [ 0 , 1 ] is called a gray level map.

For a gray level map ρ and u X , one can consider

ρ u = not ρ ( u ) X .

Given u X and α ( 0 , 1 ] , we shall use the following notations:

{ x X u ( x ) α } = not [ u ] α

and

{ x X u ( x ) > 0 } = not [ u ] .

Given u X and f : X Y , one can consider f ( u ) Y , which is described in the following way:

f ( u ) ( y ) = sup x f 1 ( { y } ) u ( x ) , if f 1 ( { y } ) 0 , if f 1 ( { y } ) = ,

for every y Y .

Given a metric space ( X , d ) and u X , we shall use the following notations:

[ u ] ¯ = not supp u

{ u X u is normal and supp u is compact } = not X

and

{ u X u is upper semicontinuous } = not X .

Given a metric space ( X , d ) , the function d : X × X [ 0 , ) , given by

d ( u , v ) = def sup α [ 0 , 1 ] h ( [ u ] α , [ v ] α ) = Lemma 2.5 from [14] sup α ( 0 , 1 ] h ( [ u ] α , [ v ] α ) ,

for every u , v X , is a distance on X . See [16] for more details.

Lemma 2.2

Let us consider a continuous function f : X X and an increasing function ρ : [ 0 , 1 ] [ 0 , 1 ] such that ρ ( 0 ) = 0 . Then

ρ ( f ( u ) ) = f ( ρ ( u ) ) ,

for every u X .

Proof

If for x X we have f 1 ( { x } ) = , then

f ( ρ ( u ) ) ( x ) = 0

and

f ( u ) ( x ) = 0 ,

so

ρ ( f ( u ) ) ( x ) = ρ ( f ( u ) ( x ) ) = ρ ( 0 ) = 0 .

Therefore,

(3) f ( ρ ( u ) ) ( x ) = ρ ( f ( u ) ) ( x ) ,

for every x X such that f 1 ( { x } ) = .

If for x X we have f 1 ( { x } ) , then

ρ ( f ( u ) ) ( x ) = ρ ( f ( u ) ( x ) ) = ρ ( sup y f 1 ( { x } ) u ( y ) ) = ρ ( sup y f 1 ( { x } ) supp u u ( y ) ) .

Since u is upper semicontinuous and f 1 ( { x } ) supp u is compact, we obtain

(4) ρ ( f ( u ) ) ( x ) = ρ ( max y f 1 ( { x } ) supp u u ( y ) ) = ρ increasing max y f 1 ( { x } ) supp u ρ ( u ( y ) ) = f ( ρ ( u ) ) ( x ) ,

for every x X such that f 1 ( { x } ) .

In view of (3) and (4), the proof is completed.□

2.3 The code space

Let us consider a nonempty set I and n N .

The set I N will be denoted by Λ ( I ) . A standard element ω of Λ ( I ) takes the form ω = ω 1 ω 2 ω n ω n + 1 .

The set I { 1 , 2 , , n } will be denoted by Λ n ( I ) . A standard element ω of Λ n ( I ) takes the form ω = ω 1 ω 2 ω n .

Given m N and ω = ω 1 ω 2 ω n ω n + 1 Λ ( I ) , the word ω 1 ω 2 ω m Λ m ( I ) will be denoted by [ ω ] m .

One can easily check that d Λ : Λ ( I ) × Λ ( I ) [ 0 , ) , given by

d Λ ( ω , θ ) = 0 , if ω = θ 1 2 min { k N ω k θ k } , if ω θ ,

for every ω = ω 1 ω 2 ω 3 ω n ω n + 1 , θ = θ 1 θ 2 θ 3 θ n θ n + 1 Λ ( I ) is a metric on Λ ( I ) .

Note that the metric space ( Λ ( I ) , d Λ ) is compact provided that I is finite.

For every i I , the function τ i : Λ ( I ) Λ ( I ) given by

τ i ( ω ) = i ω 1 ω 2 ω n ω n + 1 ,

for every ω = ω 1 ω 2 ω n ω n + 1 Λ ( I ) , is a contraction since

d Λ ( τ i ( ω ) , τ i ( θ ) ) = d Λ ( i ω , i θ ) 1 2 d Λ ( ω , θ ) ,

for every ω , θ Λ ( I ) .

2.4 Iterated function systems, iterated fuzzy function systems, orbital iterated function systems, and orbital fuzzy iterated function systems

By an iterated function system, we mean a pair ( ( X , d ) , ( f i ) i I ) = not S , where:

  • ( X , d ) is a complete metric space;

  • ( f i ) i I is a finite family of contractions f i : X X .

The fractal operator associated with S is the function F S : P c p ( X ) P c p ( X ) , given by

F S ( K ) = i I f i ( K ) ,

for all K P c p ( X ) = { A X A and A is compact } .

Let us recall that (see [1]):

  1. F S is a contraction with respect to h . As ( P c p ( X ) , h ) is a complete metric space, F S is a Picard operator. Its fixed point is denoted by A S and is called the attractor of S .

  2. For each ω Λ ( I ) , the set n N f [ ω ] n ( A S ) is a singleton and its element, denoted by a ω , belongs to A S . The function π : Λ ( I ) A S , defined by

    π ( ω ) = a ω ,

    for each ω Λ ( I ) , has the following properties:

    1. It is a continuous surjection;

    2. π τ i = f i π ,

      for each i I .

It is called the canonical projection associated with S .

By an iterated fuzzy function system, we mean a triple

( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) = not S Z , where:

  1. ( ( X , d ) , ( f i ) i I ) is an iterated function system

  2. ( ρ i ) i I is an admissible system of gray level maps, i.e., ρ i ( 0 ) = 0 , ρ i is nondecreasing and right continuous for every i I and there exists j I such that ρ j ( 1 ) = 1 .

The fuzzy Hutchinson-Barnsley operator associated with S Z is the function Z : X X , given by

Z ( u ) = i I ρ i ( f i ( u ) ) ,

for all u X .

Let us recall (see [6,7]) that Z is a Banach contraction with respect to d . As ( X , d ) is a complete metric space, Z is a Picard operator. Its unique fixed point is denoted by u S and is called the fuzzy fractal generated by S Z .

The canonical iterated fuzzy function system

( ( Λ ( I ) , d Λ ) , ( τ i ) i I , ( ρ i ) i I ) = not S Λ

will play a central role in this article.

The fuzzy Hutchinson-Barnsley operator associated with S Λ will be denoted by Z Λ and u S Λ will be denoted by u Λ . Hence,

Z Λ ( u Λ ) = u Λ

and

lim n d ( Z Λ [ n ] ( u ) , u Λ ) = 0 ,

for every u Λ ( I ) .

By an orbital iterated function system, we mean a pair ( ( X , d ) , ( f i ) i I ) = not S , where:

  1. ( X , d ) is a complete metric space;

  2. ( f i ) i I is a finite family of continuous functions f i : X X having the property that there exists C [ 0 , 1 ) such that

    d ( f i ( y ) , f i ( z ) ) C d ( y , z ) ,

    for every i I , x X and y , z O ( x ) = { x } ω Λ ( I ) , n N f [ ω ] n ( x ) .

In contrast with the case of iterated function systems, the fractal operator associated with an orbital iterated function system is a weak Picard operator. Its fixed points are called the attractors of the system.

By an orbital fuzzy iterated function system, we mean a triple ( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) = not S Z , where:

  1. ( ( X , d ) , ( f i ) i I ) is an orbital iterated function system.

  2. ( ρ i ) i I is an admissible system of gray level maps.

Let us mention that if:
  1. Z designates the fuzzy Hutchinson-Barnsley operator associated with S Z

  2. { u X for each x [ u ] there exist w x , y x X such that x , y x O ( w x ) and u ( y x ) = 1 } = not S

  3. { u S u is upper semicontinuous } = not S ,

    then Z : S S , given by

    Z ( u ) = Z ( u ) ,

    for every u S , is weak Picard and its fixed points are called fuzzy fractals generated by S Z .

For u S and x [ u ] (hence, there exist w x , y x X such that x , y x O ( w x ) and u ( y x ) = 1 ), we shall use the following notations:

lim n Z [ n ] ( u ) = not u u S ,

and

lim n Z [ n ] ( u x ) = not u x S

where u x S is described by

u x ( y ) = u ( y ) , if y O ( w x ) ¯ 0 , otherwise .

Remark 2.3

(see Lemma 3.2 from [14]). Let S Z = ( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) be an orbital fuzzy iterated function system, f : X X a continuous function and ( u j ) j J a family of elements from X having the property that there exists K P c p ( X ) such that supp u j K for all j J .

Then

f ( j J u j ) = j J f ( u j ) .

Lemma 2.4

Let S Z = ( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) be an orbital fuzzy iterated function system. Then

Z [ n ] ( u ) = ω Λ n ( I ) ρ ω ( f ω ( u ) ) ,

for every n N and every u X .

Proof

Let us consider a fixed, but arbitrarily chosen u X .

We are going to use the mathematical induction method to prove the thesis of our lemma.

For n = 1 , the thesis is valid in view of the definition of Z .

Now supposing that it is valid for n N , we have

Z [ n + 1 ] ( u ) = Z [ n ] ( Z ( u ) ) = ω Λ n ( I ) ρ ω ( f ω ( Z ( u ) ) ) = ω Λ n ( I ) ρ ω ( f ω ( i I ρ i ( f i ( u ) ) ) ) = Remark 2.3 = ω Λ n ( I ) ρ ω ( i I f ω ( ρ i ( f i ( u ) ) ) ) = ρ ω increasing and I finite = ω Λ n ( I ) i I ρ ω ( f ω ( ρ i ( f i ( u ) ) ) ) = Lemma 2.2 ω Λ n ( I ) i I ρ ω ( ρ i ( f ω ( f i ( u ) ) ) ) = ω Λ n ( I ) i I ρ ω i ( f ω i ( u ) ) = ω Λ n + 1 ( I ) ρ ω ( f ω ( u ) ) ,

i.e., the statement is valid for n + 1 .□

Theorem 2.5

(see Theorem 3.9 from [15]). Let S Z = ( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) be an orbital fuzzy iterated function system and u S . Then

u u = x [ u ] u x = x [ u ] 1 u x = max x [ u ] u x = max x [ u ] 1 u x .

3 The main results

3.1 A characterization of the fuzzy fractal u Λ

For a set I , let us consider the canonical iterated fuzzy function system S Λ = ( ( Λ ( I ) , d Λ ) , ( τ i ) i I , ( ρ i ) i I ) .

We shall denote by 1 the element of S Λ given by

1 ( ω ) = 1 ,

for every ω Λ ( I ) .

Proposition 3.1

In the aforementioned framework, we have

Z Λ [ n ] ( 1 ) ( ω ) = ρ [ ω ] n ( 1 ) ,

for every ω Λ ( I ) and every n N .

Proof

For ω Λ ( I ) , n N , and θ Λ n ( I ) , we have

τ θ ( 1 ) ( ω ) = sup α τ θ 1 ( { ω } ) 1 ( α ) , if τ θ 1 ( { ω } ) 0 , if τ θ 1 ( { ω } ) = = 1 , if [ ω ] n = θ 0 , if [ ω ] n θ ,

so we obatin

ρ θ ( τ θ ( 1 ) ) ( ω ) = ρ θ ( 1 ) , if [ ω ] n = θ ρ θ ( 0 ) = 0 , if [ ω ] n θ .

Consequently, we conclude that

Z Λ [ n ] ( 1 ) ( ω ) = Lemma 2.4 θ Λ n ( I ) ρ θ ( τ θ ( 1 ) ) ( ω ) = ρ [ ω ] n ( 1 ) .

Theorem 3.2

In the aforementioned framework, we have

u Λ = lim n u n ,

where u n S Λ is given by

u n ( ω ) = ρ [ ω ] n ( 1 ) ,

for every n N and every ω Λ ( I ) .

Proof

We have

lim n d ( Z Λ [ n ] ( 1 ) , u Λ ) = 0 ,

so, in view of Proposition 3.1, we obtain

lim n d ( u n , u Λ ) = 0 .

Remark 3.3

The aforementioned result shows that u Λ is perfectly determined by the admissible system of gray level maps ( ρ i ) i I .

3.2 A structure result concerning fuzzy fractal of a fuzzy iterated function system

Theorem 3.4

In the aforementioned framework, for every fuzzy iterated function system S Z = ( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) , we have

u S = π ( u Λ ) ,

where π is the canonical projection associated with the iterated function system ( ( X , d ) , ( f i ) i I ) .

Proof

It suffices to prove that

Z ( π ( u Λ ) ) = π ( u Λ ) .

We have

Z ( π ( u Λ ) ) ( x ) = max i I ρ i ( f i ( π ( u Λ ) ) ( x ) ) = max i I ρ i ( ( f i π ) ( u Λ ) ) ( x ) = max i I ρ i ( sup ω Λ ( I ) such that ( f i π ) ( ω ) = x u Λ ( ω ) ) = max i I ρ i ( sup ω Λ ( I ) such that ( π τ i ) ( ω ) = x u Λ ( ω ) ) = max i I ρ i ( sup θ Λ ( I ) such that π ( θ ) = x sup ω Λ ( I ) such that τ i ( ω ) = θ u Λ ( ω ) ) ,

for every x X .

As u Λ is upper semicontinuous, τ i is continuous and Λ ( I ) is compact, we infer that

Z ( π ( u Λ ) ) ( x ) = max i I ρ i ( max θ Λ ( I ) such that π ( θ ) = x τ i ( u Λ ) ( θ ) ) = ρ i is nondecreasing = max i I max θ Λ ( I ) such that π ( θ ) = x ρ i ( τ i ( u Λ ) ( θ ) ) = Lemma 2.1 = max θ Λ ( I ) such that π ( θ ) = x max i I ρ i ( τ i ( u Λ ) ( θ ) ) = sup θ Λ ( I ) such that π ( θ ) = x Z Λ ( u Λ ) ( θ ) = sup θ Λ ( I ) such that π ( θ ) = x u Λ ( θ ) = π ( u Λ ) ( x ) ,

for every x X .□

3.3 A structure result concerning the attractors of an orbital fuzzy iterated function system

Let S Z = ( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) be an orbital fuzzy iterated function system and u S .

Then for every x [ u ] , there exist w x , y x X such that x , y x O ( w x ) and u ( y x ) = 1 .

We consider the fuzzy iterated function system

( ( O ( w x ) ¯ , d ) , ( f i ) i I , ( ρ i ) i I ) = not S w x ,

where f i : O ( w x ) ¯ O ( w x ) ¯ is given by

f i ( y ) = f i ( y ) ,

for every y O ( w x ) ¯ and we denote by π x its canonical projection and by Z w x its fuzzy Hutchinson-Barnsley operator.

Let us also denote by π x ( u Λ ) the function given by

π x ( u Λ ) ( y ) = π x ( u Λ ) ( y ) , if y O ( w x ) ¯ 0 , if y X O ( w x ) ¯ .

Theorem 3.5

In the aforementioned framework, we have

u u = x [ u ] π x ( u Λ ) = x [ u ] 1 π x ( u Λ ) = max x [ u ] π x ( u Λ ) = max x [ u ] 1 π x ( u Λ ) .

Proof

Let us note that

(5) u x = π x ( u Λ ) ,

for every x [ u ] .

Indeed, we have

(6) d ( u x , π x ( u Λ ) ) d ( u x , Z [ n ] ( u x ) ) + d ( Z [ n ] ( u x ) , π x ( u Λ ) ) = d ( u x , Z [ n ] ( u x ) ) + d ( Z w x [ n ] ( u O ( w x ) ¯ ) , π x ( u Λ ) ) ,

for every n N and every x [ u ] . By passing to limit as n goes to in ( 6 ) , we conclude that u x = π x ( u Λ ) for every x [ u ] .

As, in view of Theorem 2.5, we have

u u = x [ u ] u x = x [ u ] 1 u x = max x [ u ] u x = max x [ u ] 1 u x ,

and via ( 5 ) , we obtain

u u = x [ u ] π x ( u Λ ) = x [ u ] 1 π x ( u Λ ) = max x [ u ] π x ( u Λ ) = max x [ u ] 1 π x ( u Λ ) .

4 Conclusion

In this article, we presented a structure result concerning fuzzy fractals generated by an orbital fuzzy iterated function system ( ( X , d ) , ( f i ) i I , ( ρ i ) i I ) .

In Theorem 3.4, we proved that u S = π ( u Λ ) , where π is the canonical projection associated with the iterated function system ( ( X , d ) , ( f i ) i I ) . Moreover, in Theorem 3.2, we proved that u Λ is perfectly determined by the admissible system of gray level maps ( ρ i ) i I . Finally, in Theorem 3.5, we provided a structure result concerning the fuzzy fractals generated by an orbital fuzzy iterated function system S Z .

Acknowledgments

The authors would like to express their appreciation to the reviewers of the article for their valuable and constructive suggestions. Also, the authors would like to express their gratitude to University Politehnica of Bucharest, which funded the publication of the paper.

  1. Funding information: University Politehnica of Bucharest funded the publication of the paper.

  2. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The authors state no conflict of interest.

  4. Ethical approval: The conducted research is not related to either human or animal use.

  5. Data availability statement: Data sharing is not applicable to this article as no data sets were generated or analyzed during this current study.

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Received: 2022-07-07
Revised: 2023-01-28
Accepted: 2023-03-09
Published Online: 2023-05-25

© 2023 the author(s), published by De Gruyter

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Articles in the same Issue

  1. Regular Articles
  2. A novel class of bipolar soft separation axioms concerning crisp points
  3. Duality for convolution on subclasses of analytic functions and weighted integral operators
  4. Existence of a solution to an infinite system of weighted fractional integral equations of a function with respect to another function via a measure of noncompactness
  5. On the existence of nonnegative radial solutions for Dirichlet exterior problems on the Heisenberg group
  6. Hyers-Ulam stability of isometries on bounded domains-II
  7. Asymptotic study of Leray solution of 3D-Navier-Stokes equations with exponential damping
  8. Semi-Hyers-Ulam-Rassias stability for an integro-differential equation of order 𝓃
  9. Jordan triple (α,β)-higher ∗-derivations on semiprime rings
  10. The asymptotic behaviors of solutions for higher-order (m1, m2)-coupled Kirchhoff models with nonlinear strong damping
  11. Approximation of the image of the Lp ball under Hilbert-Schmidt integral operator
  12. Best proximity points in -metric spaces with applications
  13. Approximation spaces inspired by subset rough neighborhoods with applications
  14. A numerical Haar wavelet-finite difference hybrid method and its convergence for nonlinear hyperbolic partial differential equation
  15. A novel conservative numerical approximation scheme for the Rosenau-Kawahara equation
  16. Fekete-Szegö functional for a class of non-Bazilevic functions related to quasi-subordination
  17. On local fractional integral inequalities via generalized ( h ˜ 1 , h ˜ 2 ) -preinvexity involving local fractional integral operators with Mittag-Leffler kernel
  18. On some geometric results for generalized k-Bessel functions
  19. Convergence analysis of M-iteration for 𝒢-nonexpansive mappings with directed graphs applicable in image deblurring and signal recovering problems
  20. Some results of homogeneous expansions for a class of biholomorphic mappings defined on a Reinhardt domain in ℂn
  21. Graded weakly 1-absorbing primary ideals
  22. The existence and uniqueness of solutions to a functional equation arising in psychological learning theory
  23. Some aspects of the n-ary orthogonal and b(αn,βn)-best approximations of b(αn,βn)-hypermetric spaces over Banach algebras
  24. Numerical solution of a malignant invasion model using some finite difference methods
  25. Increasing property and logarithmic convexity of functions involving Dirichlet lambda function
  26. Feature fusion-based text information mining method for natural scenes
  27. Global optimum solutions for a system of (k, ψ)-Hilfer fractional differential equations: Best proximity point approach
  28. The study of solutions for several systems of PDDEs with two complex variables
  29. Regularity criteria via horizontal component of velocity for the Boussinesq equations in anisotropic Lorentz spaces
  30. Generalized Stević-Sharma operators from the minimal Möbius invariant space into Bloch-type spaces
  31. On initial value problem for elliptic equation on the plane under Caputo derivative
  32. A dimension expanded preconditioning technique for block two-by-two linear equations
  33. Asymptotic behavior of Fréchet functional equation and some characterizations of inner product spaces
  34. Small perturbations of critical nonlocal equations with variable exponents
  35. Dynamical property of hyperspace on uniform space
  36. Some notes on graded weakly 1-absorbing primary ideals
  37. On the problem of detecting source points acting on a fluid
  38. Integral transforms involving a generalized k-Bessel function
  39. Ruled real hypersurfaces in the complex hyperbolic quadric
  40. On the monotonic properties and oscillatory behavior of solutions of neutral differential equations
  41. Approximate multi-variable bi-Jensen-type mappings
  42. Mixed-type SP-iteration for asymptotically nonexpansive mappings in hyperbolic spaces
  43. On the equation fn + (f″)m ≡ 1
  44. Results on the modified degenerate Laplace-type integral associated with applications involving fractional kinetic equations
  45. Characterizations of entire solutions for the system of Fermat-type binomial and trinomial shift equations in ℂn#
  46. Commentary
  47. On I. Meghea and C. S. Stamin review article “Remarks on some variants of minimal point theorem and Ekeland variational principle with applications,” Demonstratio Mathematica 2022; 55: 354–379
  48. Special Issue on Fixed Point Theory and Applications to Various Differential/Integral Equations - Part II
  49. On Cauchy problem for pseudo-parabolic equation with Caputo-Fabrizio operator
  50. Fixed-point results for convex orbital operators
  51. Asymptotic stability of equilibria for difference equations via fixed points of enriched Prešić operators
  52. Asymptotic behavior of resolvents of equilibrium problems on complete geodesic spaces
  53. A system of additive functional equations in complex Banach algebras
  54. New inertial forward–backward algorithm for convex minimization with applications
  55. Uniqueness of solutions for a ψ-Hilfer fractional integral boundary value problem with the p-Laplacian operator
  56. Analysis of Cauchy problem with fractal-fractional differential operators
  57. Common best proximity points for a pair of mappings with certain dominating property
  58. Investigation of hybrid fractional q-integro-difference equations supplemented with nonlocal q-integral boundary conditions
  59. The structure of fuzzy fractals generated by an orbital fuzzy iterated function system
  60. On the structure of self-affine Jordan arcs in ℝ2
  61. Solvability for a system of Hadamard-type hybrid fractional differential inclusions
  62. Three solutions for discrete anisotropic Kirchhoff-type problems
  63. On split generalized equilibrium problem with multiple output sets and common fixed points problem
  64. Special Issue on Computational and Numerical Methods for Special Functions - Part II
  65. Sandwich-type results regarding Riemann-Liouville fractional integral of q-hypergeometric function
  66. Certain aspects of Nörlund -statistical convergence of sequences in neutrosophic normed spaces
  67. On completeness of weak eigenfunctions for multi-interval Sturm-Liouville equations with boundary-interface conditions
  68. Some identities on generalized harmonic numbers and generalized harmonic functions
  69. Study of degenerate derangement polynomials by λ-umbral calculus
  70. Normal ordering associated with λ-Stirling numbers in λ-shift algebra
  71. Analytical and numerical analysis of damped harmonic oscillator model with nonlocal operators
  72. Compositions of positive integers with 2s and 3s
  73. Kinematic-geometry of a line trajectory and the invariants of the axodes
  74. Hahn Laplace transform and its applications
  75. Discrete complementary exponential and sine integral functions
  76. Special Issue on Recent Methods in Approximation Theory - Part II
  77. On the order of approximation by modified summation-integral-type operators based on two parameters
  78. Bernstein-type operators on elliptic domain and their interpolation properties
  79. A class of strongly convergent subgradient extragradient methods for solving quasimonotone variational inequalities
  80. Special Issue on Recent Advances in Fractional Calculus and Nonlinear Fractional Evaluation Equations - Part II
  81. Application of fractional quantum calculus on coupled hybrid differential systems within the sequential Caputo fractional q-derivatives
  82. On some conformable boundary value problems in the setting of a new generalized conformable fractional derivative
  83. A certain class of fractional difference equations with damping: Oscillatory properties
  84. Weighted Hermite-Hadamard inequalities for r-times differentiable preinvex functions for k-fractional integrals
  85. Special Issue on Recent Advances for Computational and Mathematical Methods in Scientific Problems - Part II
  86. The behavior of hidden bifurcation in 2D scroll via saturated function series controlled by a coefficient harmonic linearization method
  87. Phase portraits of two classes of quadratic differential systems exhibiting as solutions two cubic algebraic curves
  88. Petri net analysis of a queueing inventory system with orbital search by the server
  89. Asymptotic stability of an epidemiological fractional reaction-diffusion model
  90. On the stability of a strongly stabilizing control for degenerate systems in Hilbert spaces
  91. Special Issue on Application of Fractional Calculus: Mathematical Modeling and Control - Part I
  92. New conticrete inequalities of the Hermite-Hadamard-Jensen-Mercer type in terms of generalized conformable fractional operators via majorization
  93. Pell-Lucas polynomials for numerical treatment of the nonlinear fractional-order Duffing equation
  94. Impacts of Brownian motion and fractional derivative on the solutions of the stochastic fractional Davey-Stewartson equations
  95. Some results on fractional Hahn difference boundary value problems
  96. Properties of a subclass of analytic functions defined by Riemann-Liouville fractional integral applied to convolution product of multiplier transformation and Ruscheweyh derivative
  97. Special Issue on Development of Fuzzy Sets and Their Extensions - Part I
  98. The cross-border e-commerce platform selection based on the probabilistic dual hesitant fuzzy generalized dice similarity measures
  99. Comparison of fuzzy and crisp decision matrices: An evaluation on PROBID and sPROBID multi-criteria decision-making methods
  100. Rejection and symmetric difference of bipolar picture fuzzy graph
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