Home On the structure of self-affine Jordan arcs in ℝ2
Article Open Access

On the structure of self-affine Jordan arcs in ℝ2

  • Andrei Tetenov EMAIL logo and Allanazar Kutlimuratov
Published/Copyright: June 2, 2023
Become an author with De Gruyter Brill

Abstract

We prove that if a self-affine arc γ R 2 does not satisfy weak separation condition, then it is a segment of a parabola or a straight line. If a self-affine arc γ is not a segment of a parabola or a line, then it is a component of the attractor of a Jordan multizipper with the same set of generators.

MSC 2010: 28A80; 26A27

1 Introduction

The main question the article deals with is what may be a sufficiently general method of defining explicitly self-affine Jordan arcs in the plane and in space.

A Jordan arc γ in R n is called self-affine (resp. self-similar, self-conformal) if it is the attractor of a finite system S = { S 1 , , S m } of contracting maps of the respective type in R n . This means [1] that the arc γ is the unique nonempty compact set satisfying the equation γ = S 1 ( γ ) S m ( γ ) .

The obvious and natural way to obtain a Jordan self-similar arc γ with endpoints z 0 , z m is to build it up from pieces S k ( γ ) , which follow each other successively and are connected by common endpoints, say, S k 1 ( z m ) = S k ( z 0 ) . In this case, the maps S k should send the points z 0 , z m to the points z k 1 , z k , and the relations S i ( γ ) S j ( γ ) = if i j > 1 and S i ( γ ) S i + 1 ( γ ) = { z i } should be fulfilled. Such systems of contractions are called Jordan zippers, which were studied in detail by Aseev et al. [2]. This approach is fairly good; however, there exist examples of self-similar Jordan arcs γ = i = 1 m S i ( γ ) for which the overlaps γ i γ i + 1 are non-trivial subarcs of γ . The problem of defining parameters for fractal arcs having non-trivial overlaps is rather complicated.

We also consider a more universal setting that is applicable to each of the three previous cases.

A Jordan arc γ is called locally self-affine if, for any open subarc γ γ , there is a non-degenerate contractive affine mapping S such that S ( γ ) γ . Given a locally self-affine arc γ , the semigroup G ( γ ) = { S : S ( γ ) γ } of contractive affine maps of γ into γ is infinite, and in general case, it cannot be reduced to a finite number of generators. It is most preferable for us to be able to define such generators explicitly by some finite procedure.

The problem of finite explicit representation of self-similar and self-affine curves is closely related to the rigidity properties of these sets, which we discuss later in this section.

Self-similar curves appeared initially in the works of Peano [3] and von Koch [4] and were studied in detail by Levy [5]. Earliest examples of self-conformal sets were the limit sets of quasi-Fuchsian groups; they appeared first in 1897 in the book [6] written by Fricke and Klein. The first studies of self-affine curves were originated by de Rham [7].

These three types of sets manifest various unusual phenomena, which may be (and often are) called rigidity properties. For example, a self-similar arc γ different from a line segment cannot be shifted along itself to a small distance by a similarity close to identity [8]. Certain types of self-similar sets such as Sierpinski gasket or a fractal necklace are topologically rigid, and the only possible continuous injections of such a set K to itself are the maps sending K to some of its pieces S i 1 i n ( K ) . As it was proved by Astala [9], if the boundary of a plane domain contains a self-similar curve, then the domain is conformally rigid in the sense of Thurston [10]. There is one more property: it is well known that, for any subarc γ of a limit set Λ ( G ) of a quasi-Fuchsian group G and any bundle B of parallel lines l intersecting γ , the set { l B : # ( l γ ) = 1 } is nowhere dense in B ; this happens because loxodromic fixed points are dense in Λ ( G ) . A similar property takes place for self-similar Jordan arcs in R n [11]. If a self-similar Jordan arc γ R n contains a subarc γ admitting a bundle of parallel hyperplanes, each of which intersects γ in a unique point, then the whole γ is a straight line. If a self-similar arc is not a straight line, then it is a Whitney set of some differentiable function [12].

The geometric rigidity properties of self-similar sets were first pointed out in 1982 by Mattila [13]. He proved that if a self-similar set K in R n satisfies the open set condition, then there is the following alternative: either the set K lies on an m -dimensional affine subspace or the intersection of K with every m -dimensional C 1 -submanifold M of R n has zero Hausdorff measure H t ( E M ) , where t is the Hausdorff dimension of E .

This geometric rigidity property was extended to conformal iterated function system (IFS) in 2001 by Mauldin et al. [14]. They proved that if S = { S 1 , , S m } is a conformal IFS in R n ( n 2 ), and its attractor K is a continuum, then either dim H ( K ) > 1 or K is a proper compact segment of a geometric circle or a straight line. Further intensive work in this area was done in a cycle of works by Käenmäki [15,16].

As it follows from [13], a self-similar arc in R n belongs to class C 1 only if it is a line segment. Conversely, it was proved by Tetenov [8] that if a self-similar Jordan arc γ in R n is not a line segment, then it can be represented by some multizipper Z . Moreover [17], if such self-similar arc γ lies in the plane, then it satisfies weak separation condition. The latter statement does not hold for the arcs in R n , n 3 [18].

The situation is quite different for self-affine arcs. There are various non-trivial self-affine arcs in the plane that belong to the class C 1 . First, it was shown for the graphs of affine fractal functions in 1989 in [19,20]. Later, the theory of smooth fractal interpolation was developed by many authors [21,22].

Kravchenko (2005) studied smooth self-affine curves in the plane, considering the action of affine transformations on cones in R 2 and found the conditions under which the attractor of a self-affine zipper in the plane is a C 1 -smooth curve [23]. In 2009, Bandt and Kravchenko [24] proved that the only C 2 -differentiable self-affine arc in R 2 is a segment of a parabola or a straight line.

Another approach to the study of self-affine curves was worked out in 2006 by Protasov [25] in his research of wavelets. He considered these curves as a special case of summable fractal functions f : [ 0 , 1 ] R n . Any such function is defined as a solution in the space L p ( [ 0 , 1 ] ) of a system of m equations f ( t ) = B ˜ k ( m t + k ) ; t k m , k + 1 m , where k = 0 , , m 1 and B ˜ k is an affine operator with linear part B k . He found the conditions for smoothness of γ = f [ 0 , 1 ] in terms of eigenvalues of operators B k and proved that the smoothness class of a self-affine fractal curve in R n is either strictly smaller than n or it is infinite. In the latter case, γ is a polynomial curve of order n , which, in fact, is an affine image of a segment of the moment curve γ ( t ) = ( t , t 2 , , t n ) , t R .

In the last decade, Polikanova also proved that the moment curves in R n are the only non-degenerate C n -curves, every two oriented arcs of which are affine congruent. Her approach was purely geometrical [26,27].

Finally, in 2017, Feng and Käenmäki [28] proved a very powerful result in this series: an analytic curve in R n , n 2 , which cannot be embedded in a hyperplane, contains a non-trivial self-affine set if and only if it is an affine image of a segment of a moment curve in R n .

We put our questions in a slightly different fashion. Which conditions imply that a self-affine arc should be a parabolic segment? How a self-affine Jordan arc can be constructed, if it is not a parabolic segment? The answers are given by the following two theorems, which we prove in this article.

Theorem 1

Let γ R 2 be a locally self-affine Jordan arc, which does not satisfy weak separation condition. Then, γ is a segment of a parabola or a straight line.

Theorem 2

Let S = { S 1 , , S m } be a system of affine contraction maps in R 2 , whose attractor is a Jordan arc γ , which is not a segment of a parabola or a straight line. There is a finite affine multizipper Z = { S i j k } such that γ is the attractor of Z . All the maps from the multizipper Z are elements of the system S .

The last two theorems extend the rigidity and structural theorems for self-similar Jordan arcs proved in [8] to the self-affine case.

In Section 2, we give all necessary definitions and remind some notions and results from the study by Tetenov and Chelkanova [29].

In Section 3, we consider the ranges of transversal directions to locally self-affine arcs, proving Proposition 18.

In Subsection 3.1, we prove that for any locally self-affine Jordan arc γ , the elements of sufficiently small neighborhood of identity are the affine shifts of γ (Proposition 20) and then prove Theorem 1.

In Section 4, we prove Theorem 2.

2 Preliminaries

Zippers and multizippers. The simplest way to construct a self-similar curve is to take a polygonal line and then make iterations, replacing each of its segments by a smaller copy of the same polygonal line; this construction is called zipper [2].

Definition 3

A system S = { S 1 , , S m } of contraction mappings of R d to itself is called a zipper with vertices { z 0 , , z m } and signature ε = ( ε 1 , , ε m ) , ε i { 0 , 1 } if, for i = 1 m , S i ( z 0 ) = z i 1 + ε i and S i ( z m ) = z i ε i .

More general approach to the construction of self-similar curves and continua is provided by a graph-directed version of zippers [8], which we called multizippers.

Definition 4

Let { X u , u V } be a system of spaces, all isomorphic to R d . For each X u , let a finite array of points be given as { x 0 ( u ) , , x m u ( u ) } . Suppose for each u V and 0 k m u , we have some v ( u , k ) V and ε ( u , k ) { 0 , 1 } and a map S k ( u ) : X v X u such that

S k ( u ) ( x 0 ( v ) ) = x k 1 ( u ) or x k ( u ) and S k ( u ) ( x m v ( v ) ) = x k ( u ) or x k 1 ( u ) , depending on the signature ε ( u , r ) .

The graph-directed IFS defined by the maps S k ( u ) is called a multizipper Z .

The attractor of a multizipper Z is a system of connected and arcwise connected compact sets K u X u , satisfying the following system of equations:

K u = k = 1 m u S k ( u ) ( K v ( u , k ) ) , u V .

We call the sets K u the components of the attractor of Z .

In recent years, several authors have considered the multizippers, e.g. [30,31].

The components K u of the attractor of a multizipper Z are Jordan arcs if the following conditions are satisfied [8]:

Theorem 5

Let Z 0 = { S k ( u ) } be a multizipper with node points x k ( u ) and with a signature ε = { ( v ( u , k ) , ε ( u , k ) ) , u V , k = 1 , , m u } . If for any u V and any i , j { 1 , 2 , , m u } , the set K ( u , i ) K ( u , j ) = if i j > 1 and is a singleton if i j = 1 , then any linear parametrization { f u : I u K u } is a homeomorphism and each K u is a Jordan arc with endpoints x 0 ( u ) , x m ( u ) .

Let γ be a Jordan arc in R d . Usually, we denote its endpoints by a and b , and if x , y γ , we denote the subarc of γ with endpoints x , y by γ ( x , y ) . We define the orientation on γ by the relation x y , which is equivalent to γ ( a , x ) γ ( a , y ) .

Locally self-affine arcs and weak separation property (WSP). We say γ is locally self-affine if, for any open subarc γ γ , there is a non-degenerate contractive affine mapping S such that f ( γ ) γ .

We denote by G ( γ ) the semigroup of all non-degenerate affine contraction maps of γ into itself. Two maps f i , f j G ( γ ) are called γ -incomparable if neither f i ( γ ) f j ( γ ) nor f i ( γ ) f j ( γ ) .

We call the family ( γ ) = { f i 1 f j : f i , f j G ( γ ) , f i , f j ( γ ) are γ -incomparable } the associated family for γ . The idea of the associated family was introduced by Bandt and Graf in [32] as a tool for testing the positiveness of Hausdorff measure of self-similar sets. Our current definition is suited for locally self-affine arcs, so it differs from the one of [32]. Note that γ -incomparability does not permit ( γ ) to contain Id . We say G ( γ ) possesses WSP [33] if Id is not a limit point of ( γ ) .

Affine maps close to identity and their trajectories. Usually, in some argument, we restrict ourself to affine maps close to identity. We define a neighborhood U of the identity map Id in the group of non-degenerate affine maps G A ( R 2 ) by

U = { f ( x ) = A x + b , A G L ( 2 , R ) , A E < 1 / 2 , b R 2 , b < 1 } .

Let A ( R 2 ) be the space of all affine maps of the plane equal to g ( y ) = L y + β , where L L ( 2 , R ) and β R 2 .

We use the following lemma from our article [29].

Lemma 6

There is a homeomorphism Ψ of the set U to a neighborhood V of zero map in A ( R 2 ) such that for any f U , the map g = Ψ ( f ) satisfies the following condition: for any x R 2 , the solution y ( t ) of the Cauchy problem { y ˙ = g ( y ) , y ( 0 ) = x } is equal to f ( x ) at t = 1 .

The values of L and β for the map g ( y ) = L y + β are easily found. L = n = 1 ( 1 ) n + 1 ( A E ) n n is a matrix logarithm of A and β = n = 0 ( 1 ) n ( A E ) n n + 1 b .

The image g ( y ) = L y + β defines an affine system y ˙ = L y + β , whose evolution operator

(1) f t ( x ) = e t L x + e t L 0 t e s L d s β

assumes the value f ( x ) at t = 1 for any x , so we may write f t ( x ) = y ( t ) . Thus, the map f is included to one-parameter multiplicative group of affine maps { f t ( x ) , t R } .

This lemma allows us to include each orbit { f k ( a ) , k = 0 , , N } to a trajectory L f ( x ) = { f t ( x ) ; t R } , which is of class C .

Affine shifts and affine displacements of γ . A map f ( x ) = A x + b U is called an affine shift of the arc γ if γ γ f ( γ ) f ( γ ) and # ( γ f ( γ ) ) > 1 . We will see in Lemma 7 that f has no fixed points on γ . A map f ( x ) = A x + b U is called an affine displacement of the arc γ if f ( γ ) γ = .

Lemma 7

If g = f i 1 f j ( γ ) and g ( γ ˙ ) ( γ ˙ ) , and g preserves the orientation on γ , then g has no fixed points on γ .

Proof

Indeed, let a , b be the endpoints of γ = f i 1 f j . Let x γ ˙ be a fixed point of g . Then, say, f i ( a ) < f j ( a ) < f i ( x ) = f j ( x ) < f i ( b ) < f j ( b ) . So g ( γ ( a , x ) ) γ ( a , x ) and g 1 ( γ ( x , b ) ) γ ( x , b ) . Therefore, lim g n ( a ) = x and lim g n ( b ) = x , so x is a saddle point for g . Therefore, γ ( a , x ) and γ ( x , b ) should be non-collinear line segments, which is impossible.□

The first step for the Theorem 1 was the proof in our recent article of the following statement [29, Theorem 1(i)].

Theorem 8

Let γ = γ ( a 0 , a 1 ) be a locally self-affine Jordan arc with endpoints a 0 , a 1 in R 2 such that there is a sequence of affine shifts f k of γ converging to Id . Then γ is a parabolic or a straight line segment.

We also need the following corollary from this theorem:

Corollary 9

Let γ be a locally self-affine Jordan arc in R 2 . Let γ γ ˙ be its subarc with endpoints x 0 , x 1 . If there is a sequence of affine maps g n such that γ g n ( γ ) γ , then γ is a segment of a straight line or a parabola.

Proof

By compactness, we can choose a subsequence, denoted the same way, such that the arcs g n ( γ ) converge to some arc γ with endpoints x 0 , x 1 and γ γ γ . If there is a sequence of n such that g n 1 g n + 1 are affine shifts of γ , then γ is a segment of parabola by Theorem 8. Otherwise (by passing to a subsequence), we can assume that for any n , g n + 1 ( γ ) g n ( γ ) (or otherwise) and the fixed points y n of g n 1 g n + 1 belong to a sufficiently small subarc δ γ so that S k ( γ ) δ = for k = 1 or m . Then, the maps S k 1 g n 1 g n + 1 S k form a sequence of affine shifts of γ , converging to identity, which proves the corollary.□

3 T-ranges for Jordan arcs in the plane

Let γ be a Jordan arc in the plane. For convenience, we use complex plane notation for our argument, so we consider γ C .

Definition 10

We say that α R / π Z defines a transversal direction to the arc γ , if for any line l , which intersects real axis in the angle α , # ( γ l ) 1 .

The set T ( γ ) of all transversal directions α to the arc γ is called the range of transversal directions to γ or T-range of γ .

We say that γ has empty T-range for all subarcs if, for any non-degenerate subarc γ γ , its T-range is empty.

In other words, a Jordan arc γ C has empty T-range for all subarcs if, for any subarc γ γ and any α R / π Z , there is z γ and ρ > 0 such that z + ρ e i α γ . Therefore, the complement C T ( γ ) = R / π Z \ T ( γ ) is the set of all directions of non-degenerate chords with endpoints in γ .

Lemma 11

If γ is a locally self-affine Jordan arc in the plane, then either T ( γ ) or γ has an empty T-range for all its subarcs.

First, we prove that if γ contains no straight line segment, then C T ( γ ) is an open set.

Lemma 12

Let γ be a Jordan arc that lies completely in the upper half-plane Im z > 0 except for its end points z 0 < z 1 , which lie on the real axis. Then, for any positive r < z 1 z 0 , there are z 0 , z 1 γ such that z 1 z 0 = r .

Proof

Without loss of generality, we assume for (d1) and (d2) that z 0 < z 1 .

Take r < z 1 z 0 . The points z 0 + r and z 1 + r do not belong to γ ; therefore, there is δ > 0 such that the neighborhoods V δ ( z 0 + r ) and V δ ( z 1 + r ) are disjoint from γ . If 0 < ε < δ , then z 0 + r + i ε lies in the domain D bounded by the arc γ and a segment [ z 0 z 1 ] , while the point z 1 + r + i ε lies in the complement to the closed domain D ¯ .

Therefore, the image of γ under the translation by r + i ε intersects the arc γ . Reducing ε to 0 , we obtain that ( γ + r ) γ . This intersection does not contain points with real coordinates, and therefore, it lies in γ \ { z 0 , z 1 } . Take z 1 γ ( γ + r ) . The point z 0 = z 1 r is also in γ , which proves the lemma.□

Corollary 13

Let γ be a Jordan arc in C with endpoints z 0 , z 1 such that γ [ z 0 , z 1 ] = { z 0 , z 1 } .

Then,

  1. for any positive r < z 1 z 0 , there are z 0 , z 1 γ such that z 1 z 0 = r and Arg ( z 1 z 0 ) = Arg ( z 1 z 0 ) ;

  2. there are h , ε > 0 such that for any r < h and any θ < ε , there are z 0 , z 1 γ for which z 1 z 0 = r e i θ ( z 1 z 0 ) .

Proof

Consider the intersection of γ and the line l passing through the points z 0 z 1 . There is at least one pair of points z 0 , z 1 l such that [ z 0 , z 1 ] [ z 0 , z 1 ] and the subarc γ γ with endpoints z 0 , z 1 has no other common points with l . Applying Lemma 12 to the arc γ and the half-plane bounded by l and containing γ , we come to (d1).

Suppose for convenience that z 0 , z 1 R and z 0 < z 1 . Take some segment [ u 0 , u 1 ] ( z 0 , z 1 ) and put h = u 1 u 0 . By the compactness of [ u 0 , u 1 ] , there is λ > 0 such that a rectangle P = [ u 0 , u 1 ] × [ 0 , λ ] does not intersect γ . For any ray l + starting at the point z 0 (resp. l starting at z 1 ), which intersects both vertical sides of the rectangle P , the set l P is contained in some interval ( ξ 0 ( l ) , ξ 1 ( l ) ) for which ξ i ( l ) γ 1 , ( ξ 0 ( l ) , ξ 1 ( l ) ) γ 1 = , and ξ 0 ( l ) ξ 1 ( l ) h . Then, by (d1), for any r < h , there are z 0 , z 1 γ such that the interval [ ( z 0 , z 1 ) ] is parallel to l and z 1 z 0 = r . Take ε > 0 such that the ray l + , which forms an angle ε with ( z 0 , z 1 ) , and the ray l z 1 , which forms an angle ε with ( z 1 , z 0 ) , intersect both vertical sides of the rectangle P . Then, h and ε fit the statement (d2) of the lemma.□

Corollary 14

Let γ R 2 be a Jordan arc R 2 that does not contain a line segment. Then, T ( γ ) is a closed subarc in R / π Z .

Proof

Suppose α C T ( γ ) . Then, there is a line l that intersects γ in at least two points. The complement γ \ l is a disjoint union of subarcs with endpoints on l but no other intersection points with l . Therefore, by the statement (d2) of Corollary 13, there is a neighborhood ( α ε , α + ε ) C T ( γ ) . This shows that C T ( γ ) is open in R / π Z .

Let α , β T ( γ ) . Take a point x γ and let l α , l β be the lines passing through x in directions α and β . These lines divide the plane into four angles. The set γ \ { x } consists of two components, which are contained in two opposite angles of these four angles. As x travels along γ , these four angles remain the same; therefore, all values between α mod π and β mod π that correspond to the remaining two opposite angles belong to T ( γ ) . Since C T ( γ ) is open, T ( γ ) is a closed subarc in R / π Z .□

Lemma 15

Let γ R 2 be a Jordan arc that has empty T-range for all subarcs.

  1. For any line l R 2 , l γ is nowhere dense in l and in γ .

  2. For any line l R 2 and for any n N , the set of those lines l parallel to l for which # ( l γ ) < n is nowhere dense.

Proof

The first statement is obvious, because the set γ l is closed and does not contain any straight line interval. We prove the second statement by induction in n .

Let l be a line and let a be a vector orthogonal to l such that for any t ( 0 , 1 ) , γ ( l + t a ) . We show that the set E 1 of those t ( 0 , 1 ) for which # ( γ ( l + t a ) ) = 1 is nowhere dense in ( 0 , 1 ) . Suppose that the set E 1 is dense in some interval ( t 1 , t 2 ) ( 0 , 1 ) . This interval defines an open strip S , bounded by the lines l + t 1 a , l + t 2 a . Consider the intersection γ S = γ . Note that if for some t ( t 1 , t 2 ) , the set γ ( l + t a ) is disconnected, then it is disconnected for any t in one of the intervals ( t ε , t ] , [ t , t + ε ) for some ε > 0 . Therefore, γ is a Jordan arc, and for any t ( t 1 , t 2 ) , the intersection γ ( l + t a ) is either a point or a line segment contained in l + t a . The second case is impossible, because each line segment of that kind is a subarc in γ whose T-range is non-empty. If for each t , # ( γ ( l + t a ) ) = 1 , then T ( γ ) is non-empty.

Therefore, for any Jordan arc γ , which has empty T-range for all subarcs, and for any line l and its orthogonal vector a , the set { t : # ( γ ( l + t a ) = 1 ) } is nowhere dense in R .

Now suppose that for any subarc γ γ , the set { t : 0 < # ( γ ( l + t a ) ) < n } is nowhere dense in ( 0 , 1 ) , whereas the set { t : 0 < # ( γ ( l + t a ) ) = n } is dense in some interval ( t 1 , t 2 ) ( 0 , 1 ) . Let S be the open strip bounded by the lines l + t 1 a , l + t 2 a . Since γ intersects both these lines, one of the components of γ S is a subarc γ 0 with endpoints on different sides of S . Choose an endpoint x of this component so that both components γ 1 and γ 2 of γ \ { x } have nonempty intersection with S . The arc γ 0 is a subarc of one of these components, say, γ 1 . Suppose ( t 1 , t 2 ) ( t 1 , t 2 ) is such that for any t ( t 1 , t 2 ) , γ 2 ( l + t a ) . Being contained in the intersection of the sets { t : 0 < # ( γ 1 ( l + t a ) ) < n } and { t : 0 < # ( γ 2 ( l + t a ) ) < n } , which are both nowhere dense in ( t 1 , t 2 ) , the set { t ( t 1 , t 2 ) : # ( γ ( l + t a ) ) = n } is nowhere dense in ( t 1 , t 2 ) too.□

It follows directly from Lemma 15 that if a Jordan arc γ has empty T-range for all subarcs, then for any line l R 2 and any n N , there is a line l l , such that # ( l γ ) n .

We denote by C ( z , ρ , α ) an open half-circle { ξ = z + r e i θ , 0 < r < ρ , θ ( α π / 2 , α + π / 2 ) } .

Lemma 16

Let γ ( t ) = ( γ x ( t ) , γ y ( t ) ) , t [ 0 , 1 ] be a Jordan arc with endpoints γ ( 0 ) = ( 0 , 0 ) , γ ( 1 ) = ( 0 , h ) whose interior γ ( ( 0 , 1 ) ) lies in the open strip S = { ( x , y ) : 0 < y < h } and has empty T-range for all subarcs. Let S + be a connected component of S \ γ whose boundary contains [ 0 , + ) .

There is a point a γ and ρ > 0 such that C ( a , ρ , 0 ) S + .

Proof

Suppose max γ x ( t ) > 0 , and τ ( 0 , 1 ) satisfies γ x ( τ ) = max γ x ( t ) . Let a = γ ( τ ) . If ρ = min ( a y , 1 a y ) , then C ( a , ρ , 0 ) S + .

Suppose for any x ( 0 , 1 ) , γ x ( t ) 0 . As it follows from Lemma 15, there is a vertical line l : x = χ , χ < 0 , which intersects γ more than three times. Let S ˜ + be an unbounded component of S + \ l . The set S ˜ + \ l is an union of more than two subarcs of the arc γ . Therefore, at least one of these subarcs, say γ , has both its endpoints in l . Let a γ be the point at which γ x reaches its maximum. Then, there is such ρ , that C ( a , ρ , 0 ) S + .□

Lemma 17

Let γ ( t ) , t [ 0 , 1 ] be a Jordan arc that has empty T-range for all subarcs. Suppose γ ( 0 ) = z 0 , γ ( 1 ) = z 1 , and z 1 = z 0 + Re i α and γ ( ( 0 , 1 ) ) lies completely in an open half-plane, bounded by the line l containing z 0 , z 1 . Let D be a domain bounded by γ and [ z 0 , z 1 ] .

There are points z 0 , z 1 γ and r > 0 such that C ( z 0 , r , α ) D and C ( z 1 , r , α ) D ¯ =

Proof

Without loss of generality, we may assume that z 0 = 0 , z 1 = 1 , α = 0 , and the domain D lies in the upper half-space. Let h 2 = max γ y ( t ) and τ 0 = min { τ : γ y ( τ ) = h 2 } . Denote by γ 1 the subarc in γ with endpoints ( 0 , 0 ) and ( h 1 , h 2 ) = γ ( τ 0 ) . By Lemma 16, there exists a point a γ 1 such that C ( a , ρ , 0 ) S + . There is a ball B ( ρ , a ) such that B ( ρ , a ) γ \ γ 1 = . The set D is a component of S + \ γ whose boundary contains γ 1 , hence C ( a , ρ , 0 ) S + ( γ 1 ) . Let now τ 1 = max { τ : γ y ( τ ) = h 2 } and h 1 = γ x ( τ 1 ) . Denote by γ 2 a subarc in γ with endpoints ( 1 , 0 ) and ( h 1 , h 2 ) and let S + be an unbounded component of S + \ γ 2 . By Lemma 16, there is a point b γ 2 , for which there is a sector C ( b , ρ , 0 ) S + . Since S + D = , the same is true for C ( b , ρ , 0 ) .□

Summarizing all previous argument, we come to the following proposition.

Proposition 18

Let γ be a Jordan arc that has empty T-range for all its subarcs. For any α [ 0 , π ) , there is a subarc γ γ with endpoints z 1 , z 2 such that arg ( z 2 z 1 ) = α and γ [ z 1 z 2 ] is a closed Jordan curve bounding a domain D .

There is r > 0 and points z 0 , z 1 γ such that C ( z 0 , r , α ) D and C ( z 1 , r , α ) D ¯ = .

3.1 Arbitrary small displacements of self-affine arcs cannot be neighbor maps

Proposition 19

Let γ be a locally self-affine arc in R 2 . Suppose there is a sequence { f n } of affine displacements of γ that converges to Id . Then, T ( γ ) .

Proof

Suppose contrary. Then, γ has empty T-range for all subarcs.

Therefore, we can choose a subsequence f n = A n x + b n (denoted the same way), a point z 0 γ , and a circle V 0 = B ( z 0 , R ) , such that A n I d < 1 / 2 and fixed points of the maps or the points of invariant lines of f n are not contained in B 0 . By Lemma 6, we put into the correspondence to each of the maps f n ( x ) = A n x + b n an affine map g n ( y ) = B n y + β n such that f n ( x ) is equal to the value at t = 1 of the evolution operator φ n t ( x ) of non-homogeneous linear system y ˙ = B n y + β n . Put t n = sup { g n ( x ) , x V 0 } . Let g ˆ n ( y ) = g n ( y ) / t n .

This way we obtain a sequence of linear dynamical systems in V 0 , whose integral curves coincide with integral curves of respective systems x ˙ = g k ( x ) . At the same time, sup { g ˆ k ( x ) , x V 0 } = 1 . Due to the convexity of functions g ˆ k ( x ) , the maximum value of each of these functions is attained on the boundary of the disc V 0 .

Due to Arzelà-Ascoli theorem, the sequence g ˆ n contains a subsequence, which converges uniformly in V 0 to some affine function g 0 such that sup g 0 ( z ) on B 0 is equal to 1. Without loss of generality, we may assume that the initial sequence { g n } was chosen in such way that g ˆ n g 0 on V 0 . Since, for any of the functions, its zero value or minimal value is attained outside the disc V 0 , the value of h = g 0 ( z 0 ) cannot be equal to zero. Let α be the direction of the vector h . There is a disc V 1 with the center z 0 and a number N such that n > N and z V 1 imply g 0 ( z ) g 0 ( z 0 ) < h / 4 . Let γ 1 be a subarc in γ V 1 such that for any n > N , f n ( γ 1 ) V 1 .

Let φ n ( x , t ) be the evolution operator for the linear non-homogeneous system x ˙ = g ˆ n ( x ) . Then, for any n and z R 2 , f n ( z ) = φ n ( z , t n ) .

Since φ n ( z , t n ) z = 0 t n g ˆ n ( φ n ( z , τ ) ) d τ , the inequality

g ˆ n ( z ) g 0 ( z 0 ) g ˆ n ( z ) g 0 ( z ) + g 0 ( z ) g 0 ( z 0 ) < h / 2

implies that f n ( z ) z t n h t n h / 2 .

Therefore, for any z γ 1 , the angle between vectors h and f n ( z ) z is no greater than π / 6 .

Since the arc γ 1 has empty T-range for all its subarcs, there is a line l parallel to h , which intersects γ 1 at least at two points. As it follows from Corollary 13, there are z 1 , z 2 l γ 1 such that γ 1 ( z 1 , z 2 ) l = { z 1 , z 2 } . Let D be the domain bounded by γ 1 ( z 1 , z 2 ) [ z 1 , z 2 ] . By Lemma 17, there are the points z + , z γ 1 ( z 1 , z 2 ) and ρ > 0 such that C ( z + , r , α ) D , C ( z , r , α ) D ¯ = and C ( z , r , α ) γ = .

If we choose n such that f n ( z 0 ) z 0 < ρ / 2 , then f n ( z + ) C ( z + , r , α ) D and f n ( z ) C ( z , r , α ) C D ¯ . Therefore, f n ( γ 1 ) γ 1 , which contradicts the condition f n ( γ ) γ = .

This contradiction shows that there is a line l such that any line l parallel to l intersects γ in at most one point, so T-range T ( γ ) is non-empty.□

Proposition 20

Let γ be a locally self-affine Jordan arc in R 2 , which is not a line segment. For any sequence g n F ( γ ) , converging to Id and for any subarc γ γ , there is N such that for any n > N , g n ( γ ) γ .

Proof

Suppose contrary. Then T ( γ ) . Take a subarc γ γ and let ε be a minimal width of a of a strip S bounded by two parallel lines such that S γ . The arc γ is not a straight line, so ε > 0 . Since the sequence g n converges to Id , there is N such that for any n > N and any x γ , g n ( x ) x < ε / 2 . Take n > N and let g n = f i 1 f j , where f i and f j are affine transformations mapping γ to its subarcs f i ( γ ) and f j ( γ ) . Note that γ and g n ( γ ) are the subarcs of an arc f i 1 ( γ ) . This arc is affine equivalent to γ , and therefore, T ( f i 1 ( γ ) ) and T ( f i 1 ( γ ) ) T ( γ ) . Take α T ( f i 1 ( γ ) ) . Consider the minimal strips S 1 and S 2 bounded by pairs of parallel lines that intersect horizontal axis in the angle α and contain γ and g n ( γ ) , respectively. Since γ g n ( γ ) = , S 1 S 2 = . Take a point z γ such that d ( z , S 2 ) > ε / 2 . Since g ( z ) S 2 , g ( z ) z > ε / 2 . The obtained contradiction proves the lemma.□

Proof of Theorem 1

Let γ be a self-similar arc that does not satisfy WSP. Then, there is a sequence g n ( γ ) converging to Id . For sufficiently large n , g n U , and by Proposition 20, g n are affine shifts of γ . Therefore, by Theorem 8, the arc γ is a segment of a straight line or a parabola.□

4 Proof of Theorem 2: The partition to elementary subarcs

Let S = { S 1 , , S m } be a system of contractive affine maps in R 2 with Jordan attractor γ .

We use standard notation in this case. The set of indices { 1 , , m } is denoted by I . The subarcs S i ( γ ) are denoted by γ i . G is a semigroup, generated by { S 1 , , S m } , and the families and are defined accordingly.

Let a 0 and a 1 be the endpoints of γ . For any two points x , y γ , we write that x y , if γ ( a 0 , x ) γ ( a 0 , y ) .

We may suppose that the system S is irreducible, i.e., for any k I , i I \ { k } γ i γ . Hence, we can order the maps S 1 , , S m so that γ i γ j if and only if i j = 1 , while a 0 γ 1 and a 1 γ m .

The idea of the proof of Theorem 2 is to construct a finite set P γ , whose points a 0 = p 0 < p 1 < < p N 1 < p N = a 1 define a partition of γ to subarcs δ i , i = 1 , , N , satisfying the following conditions:

  1. For any δ i and any k = 1 , , m , there is δ j such that S k ( δ i ) δ j .

  2. For any k 1 , k 2 = 1 , , m , and for any δ i 1 , δ i 2 , S k 1 ( δ ˙ i 1 ) and S k 2 ( δ ˙ i 2 ) are either equal or disjoint.

For each g , the set γ g ( γ ) is a non-degenerate subarc, which we denote by γ g . The endpoints of γ g are the points g ( a i ) and a j , i , j { 0 , 1 } .

Let P be the set consisting of a 0 and a 1 and of points g ( a i ) , where i = 0 , 1 , g and g ( a i ) γ g γ ˙ . Let P i be the set of those p P γ ˙ , which are the endpoints of subarcs γ g that do not contain a 1 i . Thus, P = { a 0 , a 1 } P 0 P 1 .

Note two properties of the set P , which directly follow from its definition:

  1. Let g G . Then, P g ˙ ( γ ) g ( P ) .

  2. Let g 1 , g 2 G be two γ -incomparable affine maps such that g 1 ( γ ) g 2 ( γ ) is a non-degenerate subarc of γ . Then, the endpoint of the subarc g 1 ( γ ) , contained in g 2 ( γ ˙ ) , lies in g 2 ( P ) , and vice versa.

In the case when the maps g belong to S , the conditions b1 and b2 become the following ones:

  1. For any i { 1 , , m } , P γ ˙ i S i ( P ) ;

  2. For any 1 j m 1 , S j ( { a 0 , a 1 } ) γ ˙ j + 1 g j + 1 ( P ) and S j + 1 ( { a 0 , a 1 } ) γ ˙ j g j ( P )

Lemma 21

Suppose the system S = { S 1 , , S m } is irreducible. Then,

  1. the set of limit points of P is contained in { a 0 , a 1 } .

  2. there are such neighborhoods U i of the points a i , where i = 0 , 1 , that P 1 i U i = , and if for some k { 1 , m } and i , j { 0 , 1 } , S k ( a i ) = a j , then S k is a bijection of U i P i to S k ( U i ) P j .

Proof

First, we show that the set P has no limit points in γ ˙ . Suppose there is a c γ ˙ P ¯ . Then, for one of the endpoints of γ , say, a 0 , there is a sequence g n G such that g n ( a 0 ) c . It follows from Corollary 9 that γ is a segment of a parabola, which contradicts the assumptions of the lemma, so d1 is true. The same argument shows that a 1 cannot be a limit point of P 0 and a 0 cannot be a limit point of P 1 . Therefore, there are such neighborhoods U i of the points a i such that P 1 i U i = . Moreover, we choose U 0 , U 1 in such a way that γ U 0 γ 1 and γ U 1 γ m .

To check d2, we first consider the case when S 1 ( a 1 ) = a 0 . If p P 0 U 0 and p = g ( a i ) , then S 1 1 g G and S 1 1 ( p ) P 1 S 1 1 ( U 0 ) . Conversely, if p P 1 U 1 and p = g ( a i ) , then S 1 g G and S 1 ( p ) P 0 S 1 ( U 1 ) . Therefore, S 1 defines a bijection P U 0 S 1 ( U 1 ) to P U 1 S 1 1 ( U 0 ) . Enumerating all possibilities:

  1. S 1 ( a 0 ) = a 0 , S m ( a 1 ) = a 1 ;

  2. S 1 ( a 0 ) = a 0 , S m ( a 1 ) = a 0 ;

  3. S 1 ( a 0 ) = a 1 , S m ( a 1 ) = a 1 ;

  4. S 1 ( a 0 ) = a 1 , S m ( a 1 ) = a 0 ,

we find the desired pairs of neighborhoods for each of the cases.□

Lemma 22

The set P contains a finite subset P , which also satisfiesc1 andc2.

Proof

For each of the points S k ( a i ) γ ˙ , where k I and i = 0 , 1 , we denote by w ( k , i ) the connected component of the set γ k \ P , which has S k ( a i ) as its endpoint, whereas for S k ( a i ) = a j , we put w ( k , i ) = U j . Let W i = k I S k 1 ( w ( k , i ) ) U i and let P = { a 0 , a 1 } P \ ( W 0 W 1 ) .

The set P is finite, so we denote its elements by a 0 = p 0 < p 1 < < P M = a 1 , and we denote the subarcs γ ( p k 1 , p k ) by δ k .

For any j I , S j ( P ) S j ( W 0 W 1 ) S j ( P ) . At the same time, the definition of P implies that S j ( W 0 W 1 ) S j ( P ) = S j ( { a 0 , a 1 } ) . Therefore, P γ j S j ( P ) . Thus, the set P satisfies the condition c1. The condition c2 directly follows from the definition of P .□

Lemma 23

Each of the subarcs δ i , i = 1 , , M and γ i , i I is an union of subarcs S j ( δ k ) for some j I and some k { 1 , , M } whose interiors are disjoint.

Proof

The system S is irreducible, and therefore, each subarc γ j , 1 < j < m intersects two adjacent subarcs γ j 1 , γ j + 1 , so that γ j \ ( γ j 1 γ j + 1 ) . For any subarc γ ¯ j = γ j \ ( γ ˙ j 1 γ ˙ j + 1 ) , its endpoints by c2 are contained in S j ( P ) ; let them be the points S j ( p k j ) , S j ( p K j ) . The arc γ ¯ j has unique representation i = k j K j 1 S j ( δ i ) . For each of the subarcs γ j γ j + 1 , there are exactly two partitions: first, to the subarcs S j ( δ i ) and second, to the subarcs S j + 1 ( δ i ) ; choose one of them. Taking the union over all subarcs and renumerating all the points, we obtain the desired partition for the whole γ . By the property c1, the partition we obtained is at the same time a partition for each of the subarcs δ k .□

Proof of the Theorem 2

Now we can construct a Jordan multizipper, for which the components of the attractor will be the subarcs δ j . Each of the subarcs δ j , j = 1 , M , is a finite union of consequent subarcs S i ( δ k ) , which form a partition of δ j . Therefore, we can create a graph G ˜ whose vertices are u j = δ j , and an edge e i j is directed from u i to u j if there is such S k , that S k ( U j ) δ i .□

Acknowledgements

The authors thank the reviewers for their careful reading, constructive comments, and suggestions.

  1. Funding information: The work is supported by the Mathematical Center in Akademgorodok under the agreement no. 075-15-2022-281 with the Ministry of Science and Higher Education of the Russian Federation.

  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 that there is no conflict of interest.

References

[1] J. E. Hutchinson, Fractals and self-similarity, Indiana Univ. Math. J. 30 (1981), no. 5, 713–747, DOI: http://dx.doi.org/10.1512/iumj.1981.30.30055.10.1512/iumj.1981.30.30055Search in Google Scholar

[2] V. V. Aseev, A. V. Tetenov, and A. S. Kravchenko, On self-similar Jordan curves on the plane, Siberian Math. J. 44 (2003), no. 4, 481–492, DOI: https://doi.org/10.1023/A:1023848327898.10.1023/A:1023848327898Search in Google Scholar

[3] G. Peano, Sur une courbe, qui remplit toute une aire plane, Mathematische Annalen. 36 (1890), no. 1, 157–160.10.1007/BF01199438Search in Google Scholar

[4] H. von Koch, Sur une courbe continue sans tangente, obtenue par une construction geometrique elementaire, Archiv for Matemat., Astron. och Fys. 1 (1904), 681–702 .Search in Google Scholar

[5] P. Levy, Les courbes planes ou gauches et les surfaces composees de parties semblables au tout, J. Ecole Polytechn., III. Ser. 144 (1938), 227–247 et 249–291.Search in Google Scholar

[6] R. Fricke and F. Klein, Vorlesungen über die Theorie der automorphen Functionen, Teubner, Leipzig, 1897–1912.Search in Google Scholar

[7] G. de Rham, On Some Curves Defined by Functional Equations, in: Classics on Fractals, ed. Gerald A. Edgar, Addison-Wesley, 1993, pp. 285–298.Search in Google Scholar

[8] A. V. Tetenov, Self-similar Jordan arcs and graph-directed systems of similarities, Siberian Math. J. 47 (2006), no. 5, 940–949, DOI: https://doi.org/10.1007/s11202-006-0105-7.10.1007/s11202-006-0105-7Search in Google Scholar

[9] K. Astala, Self-similar zippers, in: Holomorphic Functions and Moduli, vol. 1, Springer, New York, 1988, pp. 61–73.10.1007/978-1-4613-9602-4_4Search in Google Scholar

[10] W. P. Thurston, Zippers and univalent functions, in: The Bieberbach Conjecture, Mathematical Surveys and Monographs, 21, American Mathematical Society, Providence, RI, 1986, pp. 185–197, DOI: https://doi.org/10.1090/SURV/021/15.10.1090/surv/021/15Search in Google Scholar

[11] A. V. Tetenov, On transverse hyperplanes to self-similar Jordan arcs, in: Fractals, Wavelets, and their Applications. Springer Proceedings in Mathematics & Statistics, vol. 92, Springer, Cham, 2014, pp. 147–156, DOI: https://doi.org/10.1007/978-3-319-08105-2.10.1007/978-3-319-08105-2_8Search in Google Scholar

[12] Z.-Y. Wen and L.-F. Xi, Relations among Whitney sets, self-similar arcs and quasi-arcs, Isr. J. Math. 136 (2003), 251–267, DOI: https://doi.org/10.1007/BF02807200.10.1007/BF02807200Search in Google Scholar

[13] P. Mattila, On the structure of self-similar fractals, Ann. Acad. Sci. Fenn. Ser. A I Math. 7 (1982), no. 2, 189–195.10.5186/aasfm.1982.0723Search in Google Scholar

[14] R. D. Mauldin, V. Mayer, and M. Urbański, Rigidity of connected limit sets of conformal IFSs, Michigan Math. J. 49 (2001), no. 1, 451–458, DOI: https://doi.org/10.1307/mmj/1012409964.10.1307/mmj/1012409964Search in Google Scholar

[15] A. Käenmäki, On the geometric structure of the limit set of conformal iterated function systems, Publ. Mat. 47 (2003), no. 1, 133–141.10.5565/PUBLMAT_47103_06Search in Google Scholar

[16] A. Käenmäki, Geometric rigidity of a class of fractal sets, Math. Nachr. 279 (2006), no. 1, 179–187, DOI: https://doi.org/10.1002/mana.200510354.10.1002/mana.200510354Search in Google Scholar

[17] A. V. Tetenov, On self-similar Jordan arcs on a plane, Siberian J Ind Math. 7 (2004), no. 3, 148–155 (in Russian).Search in Google Scholar

[18] A. V. Tetenov, K. G. Kamalutdinov, and D. A. Vaulin, Self-similar Jordan Arcs Which Do Not Satisfy OSC, 2016, DOI: https://doi.org/10.48550/arXiv.1512.00290.Search in Google Scholar

[19] M. F. Barnsley, Fractal functions and interpolation, Constr. Approx. 2 (1986), no. 1, 303–329, DOI: https://doi.org/10.1007/BF01893434.10.1007/BF01893434Search in Google Scholar

[20] M. F. Barnsley and A. N. Harrington, The calculus of fractal interpolation functions, J. Approx. Theory 57 (1989), no. 1, 14–34, DOI: https://doi.org/10.1016/0021-9045(89)90080-4.10.1016/0021-9045(89)90080-4Search in Google Scholar

[21] M. A. Navascués and M. V. Sebastián, Smooth fractal interpolation, J. Inequal. Appl., 2006, Article ID 78734, 1–20, DOI: https://doi.org/10.1155/JIA/2006/78734.10.1155/JIA/2006/78734Search in Google Scholar

[22] Vijay and A. K. B. Chand, Zipper fractal functions with variable scalings, Adv. Theory Nonlinear Anal. Appl. 6 (2022), no. 4, 481–501, DOI: https://doi.org/10.31197/atnaa.1149689.10.31197/atnaa.1149689Search in Google Scholar

[23] A. S. Kravchenko, Smooth self-affine curves, Sobolev Math. Inst. Prepr. no. 161, Novosibirsk, 2005, (in Russian) Available at: http://fractals.nsu.ru/info/.Search in Google Scholar

[24] C. Bandt and A. S. Kravchenko, Differentiability of fractal curves, Nonlinearity 24 (2011), no. 10, 2717–2728, DOI: https://doi.org/10.1088/0951-7715/24/10/003.10.1088/0951-7715/24/10/003Search in Google Scholar

[25] V. Yu. Protasov, Fractal curves and wavelets, Izv. Math. 70 (2006), no. 5, 975–1013, DOI: https://doi.org/10.1070/IM2006v070n05ABEH002335.10.1070/IM2006v070n05ABEH002335Search in Google Scholar

[26] I. V. Polikanova, On the curves with affine congruent arcs in affine space, Sib. Elektron. Mat. Izv. 16 (2019), 1612–1622, DOI: https://doi.org/10.33048/semi.2019.16.112.10.33048/semi.2019.16.112Search in Google Scholar

[27] I. V. Polikanova, On curves with affine-congruent arcs in an n-dimensional affine space, Siberian Math. J. 63 (2022), 180–196, DOI: https://doi.org/10.33048/smzh.2022.63.112.10.1134/S0037446622010128Search in Google Scholar

[28] D. J. Feng and A. Käenmäki, Self-affine sets in analytic curves and algebraic surfaces, Ann. Acad. Sci. Fennicae. Mathematica 43 (2016), 109–119, DOI: https://doi.org/10.5186/aasfm.2018.4306.10.5186/aasfm.2018.4306Search in Google Scholar

[29] A. V. Tetenov and O. A. Chelkanova, Rigidity theorem for self-affine arcs, Dokl. Math. 103 (2021), no. 2, 81–84, DOI: https://doi.org/10.1134/S1064562421020058.10.1134/S1064562421020058Search in Google Scholar

[30] H. Rao and S.-Q. Zhang, Space-filling curves of self-similar sets(I), Nonlinearity 29 (2016), 2112–2132, DOI: https://doi.org/10.1088/0951-7715/29/7/2112.10.1088/0951-7715/29/7/2112Search in Google Scholar

[31] J. Ventrella, Brainfilling Curves-a Fractal Bestiary, (2012), Lulu.com.Search in Google Scholar

[32] C. Bandt and S. Graf, Self-similar sets 7. A characterization of self-similar fractals with positive Hausdorff measure, Proc. Amer. Math. Soc. 114 (1992), no. 4, 995–1001, DOI: https://doi.org/10.2307/2159618.10.1090/S0002-9939-1992-1100644-3Search in Google Scholar

[33] M. P. W. Zerner, Weak separation properties for self-similar sets, Proc. Amer. Math. Soc. 124 (1996), no. 11, 3529–3539.10.1090/S0002-9939-96-03527-7Search in Google Scholar

Received: 2022-12-20
Revised: 2023-04-05
Accepted: 2023-04-12
Published Online: 2023-06-02

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

This work is licensed under the Creative Commons Attribution 4.0 International License.

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
Downloaded on 8.10.2025 from https://www.degruyterbrill.com/document/doi/10.1515/dema-2022-0228/html?lang=en
Scroll to top button