Misiurewicz point

Misiurewicz point

A Misiurewicz point is a parameter in the Mandelbrot set (the parameter space of quadratic polynomials) for which the critical point is strictly preperiodic (i.e., it becomes periodic after finitely many iterations but is not periodic itself). By analogy, the term Misiurewicz point is also used for parameters in a Multibrot set where the unique critical point is strictly preperiodic. (This term makes less sense for maps in greater generality that have more than one (free) critical point because some critical points might be periodic and others not.)


Mathematical notation

A parameter c is a Misiurewicz point M_{k,n} \, if it satisfies the equations

f_c^{(k)}(z_{cr}) = f_c^{(k+n)}(z_{cr}) \,


 f_c^{(k-1)}(z_{cr}) \neq f_c^{(k+n-1)}(z_{cr})\,

so :

M_{k,n} = c : f_c^{(k)}(z_{cr}) = f_c^{(k+n)}(z_{cr}) \,

where :

and  f_c^{k} denotes the k-th iterate of fc.


Misiurewicz points are named after the Polish-American mathematician Michał Misiurewicz.[1]

Note that the term "Misiurewicz point" is used ambiguously: Misiurewicz originally investigated maps in which all critical points were non-recurrent (that is, there is a neighborhood of every critical point that is not visited by the orbit of this critical point), and this meaning is firmly established in the context of dynamics of iterated interval maps.[2] The case that for a quadratic polynomial the unique critical point is strictly preperiodic is only a very special case; in this restricted sense (as described above) this term is used in complex dynamics; a more appropriate term would be Misiurewicz-Thurston points (after William Thurston who investigated postcritically finite rational maps).

A complex quadratic polynomial has only one critical point. By a suitable conjugation any quadratic polynomial can be transformed into a map of the form  P_c(z)=z^2+c \, which has a single critical point at  z = 0\,. The Misiurewicz points of this family of maps are roots of the equations

P_c^{(k)}(0) = P_c^{(k+n)}(0),

(subject to the condition that the critical point is not periodic), where :

  • k is the pre-period
  • n is the period
  • P_c^{(n)} = P_c ( P_c^{(n-1)})\, denotes the n-fold composition of P_c(z)=z^2+c\, with itself i.e. the nth iteration of P_c\,.

For example, the Misiurewicz points with k=2 and n=1, denoted by M2,1, are roots of

P_c^{(2)}(0) = P_c^{(3)}(0)
\Rightarrow c^2+c=(c^2+c)^2+c
\Rightarrow c^4+2c^3=0.

The root c=0 is not a Misiurewicz point because the critical point is a fixed point when c=0, and so is periodic rather than pre-periodic. This leaves a single Misiurewicz point M2,1 at c = −2.

Properties of Misiurewicz points of complex quadratic mapping

Misiurewicz points belong to the boundary of the Mandelbrot set. Misiurewicz points are dense in the boundary of the Mandelbrot set.[3][4]

If c\, is a Misiurewicz point, then the associated filled Julia set is equal to the Julia set, and means the filled Julia set has no interior.

If c\, is a Misiurewicz point, then in the corresponding Julia set all periodic cycles are repelling (in particular the cycle that the critical orbit falls onto).

Mandelbrot set and Julia set J_c\, are locally asymptotically similar around Misiurewicz points. Mandelbrot set is self-similar around Misiurewicz points [5]


Misiurewicz points can be classified according to number of external rays that land on them :[3]

  • branch points ( = points that disconnect the Mandelbrot set into at least three components.) with 3 or more external arguments ( angles )
  • non-branch points with exactly 2 external arguments ( = interior points of arcs within the Mandelbrot set) : these points are less conspicuous and thus not so easily to find on pictures.
  • end points with 1 external argument

According to the Branch Theorem of the Mandelbrot set,[4] all branch points of the Mandelbrot set are Misiurewicz points (plus, in a combinatorial sense, hyperbolic components represented by their centers).[3][4]

Many (actually, most) Misiurewicz parameters in the Mandelbrot set look like `centers of spirals'.[6] The explanation for this is the following: at a Misiurewicz parameter, the critical value jumps onto a repelling periodic cycle after finitely many iterations; at each point on the cycle, the Julia set is asymptotically self-similar by a complex multiplication by the derivative of this cycle. If the derivative is non-real, then this implies that the Julia set, near the periodic cycle, has a spiral structure. A similar spiral structure thus occurs in the Julia set near the critical value and, by Tan Lei's aforementioned theorem, also in the Mandelbrot set near any Misiurewicz parameter for which the repelling orbit has non-real multiplier. Depending on the value of the multiplier, the spiral shape can seem more or less pronounced. The number of the arms at the spiral equals the number of branches at the Misiurewicz parameter, and this equals the number of branches at the critical value in the Julia set. (Even the `principal Misiurewicz point in the 1/3-limb', at the end of the parameter rays at angles 9/56, 11/56, and 15/56, turns out to be asymptotically a spiral, with infinitely many turns, even though this is hard to see without maginification.)

External arguments

External arguments of Misiurewicz points, measured in turns are :

  • rational numbers
  • proper fraction with even denominator
    • dyadic fractions with denominator  = 2^b\, and finite ( terminating ) expansion , like :
\frac{1}{2}_{10} = 0.5_{10} =   0.1_2 \,
\frac{1}{6}_{10} = \frac{1}{2*3}_{10}= 0,16666..._{10} = 0.0(01)..._2\,.[7]

where :

a and b are positive integers and b is odd ,

subscript number shows base of numeral system.

Examples of Misiurewicz points of complex quadratic mapping

End points

Orbit of critical point z = 0\, under  f_{-2}\,
 c =M_{2,1}\,

Point c =  M_{2,2} = i \,  :

  • is a tip of the filament[8]
  • Its critical orbits is  \{0, i, i-1, -i, i-1, -i...\} \, [9]

Point  c = M_{2,1} = -2\,

Notice that it is z-plane (dynamical plane) not c-plane (parameter plane) and point  z = -2\, is not the same point as  c = -2\,.

Point  c = -2 =M_{2,1}\, is landing point of only one external ray ( parameter ray) of angle 1/2 .

Non-Branch points

 c =M_{23,3}\,

Point c= -0.77568377+0.13646737*i \, is near a Misiurewicz point M_{23,2}\,. It is

  • a center of a two-arms spiral
  • a landing point of 2 external rays with angles : \frac{8388611}{25165824}\, and \frac{8388613}{25165824}\, where denominator is 3*2^{23}\,
  • preperiodic point with preperiod k = 23\, and period n = 2\,

Point c = -1.54368901269109 \, is near a Misiurewicz point M_{3,2}\, ,

  • which is landing point for pair of rays : \frac{5}{12}\, , \frac{7}{12}\,
  • has preperiod k = 3\, and period n = 2\,

Branch points

 c =M_{4,1}\,

Point  c = -0.1010... +0.9562...*i =M_{4,1}\, is a principal Misiurewicz point of the 1/3 limb. It has 3 external rays 9/56, 11/56 and 15/56.

See also

  1. ^ Michał Misiurewicz home page, Indiana University-Purdue University Indianapolis
  2. ^ Wellington de Melo, Sebastian van Strien, "One-dimensional dynamics". Monograph, Springer Verlag (1991)
  3. ^ a b c Adrien Douady, John Hubbard, "Etude dynamique des polynômes complexes", prépublications mathématiques d'Orsay, 1982/1984
  4. ^ a b c Dierk Schleicher, "On Fibers and Local Connectivity of Mandelbrot and Multibrot Sets", in: M. Lapidus, M. van Frankenhuysen (eds): Fractal Geometry and Applications: A Jubilee of Benoît Mandelbrot. Proceedings of Symposia in Pure Mathematics 72, American Mathematical Society (2004), 477–507 or online paper from arXiv.org
  5. ^ Lei.pdf Tan Lei, "Similarity between the Mandelbrot set and Julia Sets", Communications in Mathematical Physics 134 (1990), pp. 587-617.
  6. ^ The boundary of the Mandelbrot set by Michael Frame, Benoit Mandelbrot, and Nial Neger
  8. ^ Tip of the filaments by Robert P. Munafo
  9. ^ a b Preperiodic (Misiurewicz) points in the Mandelbrot se by Evgeny Demidov
  10. ^ tip of main antennae by Robert P. Munafo

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