Mandelbrot set and Julia sets of fractional order Marius-F. Danca STAR-UBB Institute

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Mandelbrot set and Julia sets of fractional order
Marius-F. Danca
STAR-UBB Institute,
Babes-Bolyai University,
400084, Cluj-Napoca, Romania
and
Romanian Institute of Science and Technology,
400487, Cluj-Napoca, Romania
danca@rist.ro
and
Michal Feˇckan
Faculty of Mathematics, Physics and Informatics,
Comenius University in Bratislava,
84215 Bratislava, Slovakia
and
Mathematical Institute, Slovak Academy of Sciences,
84104 Bratislava, Slovakia
michal.feckan@gmail.com
October 6, 2022
Abstract
In this paper the fractional-order Mandelbrot and Julia sets in the sense of q-th Caputo-
like discrete fractional differences, for q(0,1), are introduced and several properties are
analytically and numerically studied. Some intriguing properties of the fractional models are
revealed. Thus, for q1, contrary to expectations, it is not obtained the known shape of the
Mandelbrot of integer order, but for q0. Also, we conjecture that for q0, the fractional-
order Mandelbrot set is similar to the integer-order Mandelbrot set, while for q0 and c= 0,
one of the underlying fractional-order Julia sets is similar to the integer-order Mandelbrot set.
In support of our conjecture, several extensive numerical experiments were done. To draw the
Mandelbrot and Julia sets of fractional order, the numerical integral of the underlying initial
values problem of fractional order is used, while to draw the sets, the escape-time algorithm
adapted for the fractional-order case is used. The algorithm is presented as pseudocode.
keywords: Mandelbrot set of fractional order; Julia set of fractional order; Caputo-like
discrete fractional difference
1
arXiv:2210.02037v1 [nlin.CD] 5 Oct 2022
1 Introduction
The study of the dynamics of complex maps was initiated by P. Fatou and G. Julia in the early of
twentieth century, before being revived by B. Mandelbrot. As know, in the complex plane C, the
Integer Order (IO) Mandelbrot set represents the set of complex numbers (parameters) cfor which
the quadratic map fc(z) = z2+c(Mandelbrot map) does not diverge to infinity when it is iterated
with fcfrom z= 0. This set, has been first defined and drawn by Robert W. Brooks and Peter
Matelski in 1978 [1], and later made famous by Benoit Mandelbrot (see e.g. [2]). The dynamics
generates by fcrepresent a huge sources of fractal structures (see e.g. [3, 4, 5, 6]).
Julia sets are made of all points which under iterations do not go to an attractor which may be
at infinity. Compared to Mandelbrot set, where cis variable in the parametric plane C, Julia sets
are obtained for fixed cand the origin of iterations variable in C.
The Mandelbrot set is known as the set of all points cfor which Julia sets are compact and
connected.
Details and background on Mandelbrot set and Julia sets can be found in the following works
[2, 7, 8, 9, 10, 3, 11], to cite only few of them.
Due the description of memory and hereditary properties, Fractional Order (FO) difference
equations still receive increasing attention. However, as mentioned in [12], overall, fractional calculus,
closely related to classical calculus, is not direct generalization of classical calculus in the sense
of rigorous mathematics. One of the first definitions of a fractional difference operator has been
proposed in 1974 [13]. While there are many works on fractional differential equations, there still
are only few works in the theory of the fractional finite difference equations. In [14, 15, 16] problems
related to Caputo fractional sums and differences can be found, while in [29] Initial Value Problems
(IVPs) in fractional differences are studied. For stability of fractional differences compare [17, 18],
while properties of fractional discrete logistic map, weakly fractional difference equations, symmetry-
breaking of fractional maps can be found in [19, 20, 21]. The nonexistence of periodic solutions in
fractional difference equations is analyzed in [22].
Notations utilized in this paper:
IOM: Mandelbrot of IO;
IOKc: Filled Julia set of IO;
IOJc: Julia set of IO;
F OM: Mandelbrot set of FO;
F OKc: Filled Julia set of FO;
DEM: Distance Estimator Method;
IIM: Inverse Iteration Method
2 Mandelbrot set and Julia sets of integer order
In this section, few of the most important characteristics of IOMset, and IOKcsets, which will
be revealed analytically or numerically in the cases of Mandelbrot and Julia sets of FO, are briefly
presented.
The iteration of fcis obtained by the relation
zn=z2
n1+c, z0= 0, n N={1,2, ...},(1)
which generates the sequence
z0= 0, z1=fc(0) = c, z2=f2
c(0) = c2+c, z3=f3
c(0) = (c2+c)2+c, ... (2)
2
where by fk
c(0) one understands fc(fk1
c(0)).
A complex number cIOMset if the absolute value of znin the sequence (2) remains bounded
for all nN,|zn|<2, for all n0.
As proposed by Mandelbrot, the boundary of the Mandelbrot set represents a fractal curve (Fig.
1 (a)). For the history related to the origin of the IOMset compare [23].
Consider the set of all points z0which tend to through the iteration (1)
Ac() = {z0C:fk
c(z0)→ ∞,as k→ ∞}.
The set Ac() depends on c, and his frontier represents the IOJcset of fc.
The filled Julia set for fixed c, of IO, related to fc,IOKcwhich, for computationally reasons is
considered in this paper, is the set of all points z0Cfor which the orbit (2) is bounded
IOKc=C\Ac() = {z0C:fk
c(z0) remains bounded for all k}.
The IOJcset is contained in the IOKcset and is the boundary of the IOKcset
IOKc=IOJc=Ac().
In this paper, beside some new properties related to the Mandelbrot set of FO, the following
known properties of Mandelbrot set and Julia sets of IO will be analytically or numerically studied
on their FO counterparts.
1. The IOKcsets for purely real c, and IOMset, are symmetric about the real axis (reflection
symmetry). Julia sets of fcare symmetric about the origin.
2. As known, it is conjectured that the Mandelbrot set is locally connected [7, 23], the full conjec-
ture of this very technical and complicated property being still open. Mandelbrot had decided
empirically that his isolated islands were actually connected to the mainland by very thin fil-
aments [24]. In this paper we are interested in the connectivity property as a computationally
property which by using, beside the escape-time algorithm (see Appendix A), a performing
method (Distance Estimator Method), revel the filaments connecting the apparently isolated
islands to the mainland of the Mandelbrot set or Julia sets, of IO or FO. Empirical small areas
are considered.
3. The IOMset is the set of all parameters cfor which IOKcare connected sets;
4. The F OMset is bounded;
5. For csituated outside of IOMone obtains Cantor sets (“dust” sets composed of infinitely
disjoint points);
6. The Julia sets can be connected, disconnected or totally disconnected (see e.g. [25, 26, 27]).
To note that the IOMset represents the set of all points in the complex plane for which the
alternated Julia sets [28] are disconnected (but not totally disconnected).
In this paper the filled Julia sets are considered.
Hereafter, by point in the complex plane, one understands the image in the complex plane of a
complex number.
Drawing Mandelbrot set and Julia sets of IO and FO, bases on the theorem which states that
iterating fc, with starting value z0, only one of the following possibilities happens: either the obtained
orbit remains bounded by 2, or diverges to [5].
3
In Fig. 1 (a) is presented the IOMset, while in Figs. 1 (c)-(j) there are presented several
IOKcsets for different cvalues. In Fig. 1 (c), there is presented an IOJcset with no interior, with
c= 0.359 + ı0.599, while in Fig.1 (d) there are presented comparatively, both the IOKcand IOJc
sets for the same value of parameter c= 0.276 + ı0.536, obtained with the time-escape algorithm
and IIM, [5], respectively.
3 Fractional Order Mandelbrot map
In this section the fractional discretization of the Mandelbrot and Julia sets of FO, in the sense of
Caputo-like are introduced.
To obtain the fractional discretization of the F OM, consider the time scale Na={a, a +
1, a + 2, ...}. For q > 0 and q6∈ Nthe q-th Caputo-like discrete fractional difference of a function
u:NaRis defined as is defined [29, 30] as
q
au(t)=∆(nq)
anu(t) = 1
Γ(nq)
t(nq)
X
s=a
(ts1)(nq1)nu(s),(3)
for tNa+nqand n= [q] + 1.
nis the n-th order forward difference operator,
nu(s) =
n
X
k=0 n
k(1)nku(s+k),
while ∆q
arepresents the fractional sum of order qof u, namely,
q
au(t) = 1
Γ(q)
tq
X
s=a
(ts1)(q1)u(s), t Na+q,
with the falling factorial t(q)in the following form:
t(q)=Γ(t+ 1)
Γ(tq+ 1).
The fractional operator ∆q
amaps functions defined on Nato functions on Na+q(for time scales
see, e.g., [31]).
For the case considered in this paper, q(0,1), when ∆u(s) = u(s+ 1) u(s), n= 1, and
starting point a= 0, q-th Caputo’s fractional derivative, ∆q, becomes
qu(t) = 1
Γ(1 q)
t(1q)
X
s=a
(ts1)(q)u(s).(4)
Consider next, the FO autonomous IVP in the sense of Caputo’s derivative
qu(t) = f(u(t+q1)), t N1q, u(0) = u0,(5)
with fa continuous real valued map and q(0,1). The numerical solution is
u(t) = u0+1
Γ(q)
tq
X
s=1q
(ts1)(q1)f(u(s+q1)),(6)
4
摘要:

MandelbrotsetandJuliasetsoffractionalorderMarius-F.DancaSTAR-UBBInstitute,Babes-BolyaiUniversity,400084,Cluj-Napoca,RomaniaandRomanianInstituteofScienceandTechnology,400487,Cluj-Napoca,Romaniadanca@rist.roandMichalFeckanFacultyofMathematics,PhysicsandInformatics,ComeniusUniversityinBratislava,84215...

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