Limits of quadratic rational maps with degenerate parabolic fixed - - PowerPoint PPT Presentation

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Limits of quadratic rational maps with degenerate parabolic fixed - - PowerPoint PPT Presentation

Limits of quadratic rational maps with degenerate parabolic fixed points of multiplier e 2 i / q 1 Xavier Buff joint work with Jean calle and Adam Epstein 26 novembre 2010 X. Buff Limits of degenerate parabolics Degenerate parabolic


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Limits of quadratic rational maps with degenerate parabolic fixed points of multiplier e2πi/q → 1

Xavier Buff joint work with Jean Écalle and Adam Epstein 26 novembre 2010

  • X. Buff

Limits of degenerate parabolics

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Degenerate parabolic fixed points

Let f : P1 → P1 be a rational map. A fixed point of f is parabolic if the multiplier is a root of unity. If the multiplier is e2πip/q and ζ is a coordinate vanishing at the fixed point, then ζ ◦ f ◦q = e2πip/qζ · (1 + ζνq) + O(ζνq+2) for some integer ν ≥ 1. The fixed point is a degenerate parabolic fixed point if ν ≥ 2.

  • X. Buff

Limits of degenerate parabolics

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Families of quadratic rational maps

Consider the quadratic rational map fa,p/q : z → e2πip/q z 1 + az + z2 which fixes 0 with multiplier e2πip/q. Question What can we say regarding the set Ap/q of points a ∈ C for which fa,p/q has a degenerate parabolic fixed point at 0 ?

  • X. Buff

Limits of degenerate parabolics

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Pictures

The bifurcation locus Bp/q is the closure of the set of parameters a ∈ C for which fa,p/q has a parabolic cycle of period > 1. Ap/q ⊂ Bp/q.

  • X. Buff

Limits of degenerate parabolics

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Pictures

B0/1

  • X. Buff

Limits of degenerate parabolics

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SLIDE 6

Pictures

B1/5

  • X. Buff

Limits of degenerate parabolics

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SLIDE 7

Pictures

B1/10

  • X. Buff

Limits of degenerate parabolics

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SLIDE 8

Pictures

B1/20

  • X. Buff

Limits of degenerate parabolics

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SLIDE 9

Pictures

B1/50

  • X. Buff

Limits of degenerate parabolics

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SLIDE 10

Pictures

B0/1

  • X. Buff

Limits of degenerate parabolics

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The cardinality of Ap/q

as z → ∞, we have f ◦q

a,p/q(z) = z ·

  • 1 + Cp/q(a)zq

+ O(zq+1). a ∈ Ap/q if and only if Cp/q(a) = 0. Proposition Cp/q is a polynomial of degree q − 2 having only simple roots. The degree q − 2 is obtained by studying the behaviour as a → ∞. The simplicity of roots is a transversality statement which we shall not study today.

  • X. Buff

Limits of degenerate parabolics

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SLIDE 12

Limits as 1/q → 0

It is tempting to conjecture that the sets B1/q have a Hausdorff limit in C ∪ {∞}. This is still unknown. It is tempting to conjecture that the sets A1/q have a Hausdorff limit in C ∪ {∞}. This is almost known. Proposition There exists an entire function C with the following properties. C has order of growth 1. More precisely, as b → ∞ log |C(b)| ∈ O(|b| log |b|) \ O(|b|). In particular C has infinitely many zeroes. the set A of points a ∈ C such that C(1/a2) = 0 satisfies A ∪ {0} ⊆ lim inf

q→∞ A1/q

and lim sup

q→∞

A1/q ⊆ A ∪ {0, ∞}.

  • X. Buff

Limits of degenerate parabolics

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Changes of coordinates

It is convenient to introduce the rational map Gb : w → w + 1 + b w . If b = 1/a2, then Fa,0 is conjugate to Gb via w = a/z.

  • X. Buff

Limits of degenerate parabolics

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Ecalle-Voronin invariants

Attracting Fatou coordinates : Φb,att(w) = lim

n→+∞ G◦n b (w) − n − b · n

  • k=1

1 k . Repelling Fatou parameterization : Ψb,rep(w) = lim

n→+∞ G◦n b

  • w − n + b ·

n

  • k=1

1 k

  • .

Voronin invariants :

b (w) = Φb,att ◦ Ψb,rep(w).

  • X. Buff

Limits of degenerate parabolics

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The function C

  • E+

b = Id +

  • k≥0

ck(b)e2πikw and

  • E−

b = Id +

  • k≤0

ck(b)e2πikw with ck entire functions of b. The entire function C is the Fourier coefficient : C = c1.

  • X. Buff

Limits of degenerate parabolics

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Hypertangents and multizetas

Hypertangents : Pe1 = π cot(πw) =

  • k∈Z

1 k + w and Pen =

  • k∈Z

1 (k + w)n . Multizetas : ζ(s1, . . . , sr) =

  • 0<nr<...<n2<n1<∞

1 nsr

r

· · · 1 ns2

2

· 1 ns1

1

.

  • X. Buff

Limits of degenerate parabolics

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Expansion with respect to b

b = id + be1 + b2e2 + b3e3 + . . .

with e1 = Pe1 e2 = 0 e3 = 3ζ(3)Pe2 e4 = −ζ(4)Pe3 + 10ζ(5)Pe2

  • X. Buff

Limits of degenerate parabolics

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Order of growth

  • E+

b in the upper half-plane ℑ(w) > h+ b with h+ b comparable

to ℑ(b) log |b|.

  • E−

b in the lower half-plane ℑ(w) < h− b with h− b comparable

to ℑ(b) log |b|. This is obtained by comparing the dynamics of Gb to the real flow of the vector field

  • 1 + b

w

  • d

dw . The Koebe 1/4-Theorem implies that log |C(b)| ≤ 1 4 · h+

b

2π = O(|b| log |b|).

  • X. Buff

Limits of degenerate parabolics

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Order of growth

Assume ℜ(b) = 1/2. Gb has a indifferent fixed point at −b and so, the basin of ∞ only contains 1 critical point. There is a univalent map χ : {ℑ(w) > 0} → {ℑ(w) > h−

b }

satisfying χ(w + 1) = χ(w) + 1 and a translation T such that

  • E1/4 = T ◦

E+

b ◦ χ.

According to the Fatou-Shishikura Inequality for Finite Type Maps, c1(1/4) = 0. log |C(b)| ≥ 2πh−

b + log

  • c1(1/4)
  • .
  • X. Buff

Limits of degenerate parabolics

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Pictures again

1/4 sends each red tile univalently to a upper half-plane and

each yellow tile univalently to a lower half-plane.

  • X. Buff

Limits of degenerate parabolics

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SLIDE 21

Pictures again

1/2+10i sends each red tile univalently to a upper half-plane

and each yellow tile univalently to a lower half-plane.

  • X. Buff

Limits of degenerate parabolics