Germs of analytic families of diffeomorphisms unfolding a parabolic - - PowerPoint PPT Presentation

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Germs of analytic families of diffeomorphisms unfolding a parabolic - - PowerPoint PPT Presentation

Germs of analytic families of diffeomorphisms unfolding a parabolic point (I) Christiane Rousseau Work done with C. Christopher, P. Marde si c, R. Roussarie and L. Teyssier 1 Minicourse 1, Toulouse, November 2010 Structure of the


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Germs of analytic families of diffeomorphisms unfolding a parabolic point (I)

Christiane Rousseau

Work done with C. Christopher, P. Mardeˇ si´ c, R. Roussarie and L. Teyssier

1 Minicourse 1, Toulouse, November 2010

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Structure of the mini-course

◮ Statement of the problem (first lecture) ◮ The preparation of the family (first lecture) ◮ Construction of a modulus of analytic classification in

the codimension 1 case (second lecture)

◮ The realization problem in the codimension 1 case

(third lecture)

2 Minicourse 1, Toulouse, November 2010

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Statement of the problem We consider germs of generic k-parameter families fǫ of diffeomorphisms unfolding a parabolic point of codimension k f0(z) = z+zk+1 +o(zk+1) When are two such germs conjugate?

3 Statement of the problem Minicourse 1, Toulouse, November 2010

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Conjugacy of two germs of families Two germs of families of diffeomorphisms fǫ and ˜ f˜

ǫ are conjugate it there exists r,ρ > 0 and

analytic functions h : Dρ → C, H : Dr ×Dρ → C such that

◮ h is a diffeomorphism and for each fixed ǫ,

Hǫ = H(·,ǫ) is a diffeomorphism;

◮ for all ǫ ∈ Dρ and for all z ∈ Dr, then

˜ fh(ǫ) = Hǫ ◦fǫ ◦(Hǫ)−1

4 Statement of the problem Minicourse 1, Toulouse, November 2010

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The choice of Dr Dr is chosen so that the behaviour of f0 on the boundary is as in

5 Statement of the problem Minicourse 1, Toulouse, November 2010

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The choice of Dr Dr is chosen so that the behaviour of f0 on the boundary is as in Dρ is chosen sufficiently small so that fǫ has the same behaviour near the boundary. In particular, all fixed points of fǫ remain inside the disk.

6 Statement of the problem Minicourse 1, Toulouse, November 2010

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A natural strategy: the use of normal forms A germ of generic k-parameter family fǫ unfolding a parabolic point of codimension k is formally conjugate to the time-1 map of a vector field vǫ = Pǫ(z) 1+a(ǫ)zk ∂ ∂z where Pǫ(z) = zk+1 +ǫk−1zk−1 +···+ǫ1z+ǫ0

7 Statement of the problem Minicourse 1, Toulouse, November 2010

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A natural strategy: the use of normal forms A germ of generic k-parameter family fǫ unfolding a parabolic point of codimension k is formally conjugate to the time-1 map of a vector field vǫ = Pǫ(z) 1+a(ǫ)zk ∂ ∂z where Pǫ(z) = zk+1 +ǫk−1zk−1 +···+ǫ1z+ǫ0 Problem: the change to normal form diverges. What does it mean?

8 Statement of the problem Minicourse 1, Toulouse, November 2010

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Can we exploit the formal normal form despite its divergence? Let us look at the case k = 1: vǫ = z2 −ǫ 1+a(ǫ)z ∂ ∂z

9 Statement of the problem Minicourse 1, Toulouse, November 2010

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Can we exploit the formal normal form despite its divergence? Let us look at the case k = 1: vǫ = z2 −ǫ 1+a(ǫ)z ∂ ∂z Two singular points ±√ǫ with eigenvalues µ± = ±2√ǫ 1±a(ǫ)√ǫ

10 Statement of the problem Minicourse 1, Toulouse, November 2010

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The parameter is an analytic invariant of the vector field! Indeed, we have 1 µ+ + 1 µ− = a(ǫ) 1 µ+ − 1 µ− = 1 √ǫ

11 Statement of the problem Minicourse 1, Toulouse, November 2010

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Hence, can we hope to bring the system to a “prenormal” form in which the parameter is invariant?

12 Statement of the problem Minicourse 1, Toulouse, November 2010

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Hence, can we hope to bring the system to a “prenormal” form in which the parameter is invariant?

Yes!

This is the preparation part.

13 Statement of the problem Minicourse 1, Toulouse, November 2010

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Hence, can we hope to bring the system to a “prenormal” form in which the parameter is invariant?

Yes!

This is the preparation part.

Advantage: a conjugacy between prepared families must preserve the canonical parameters.

14 Statement of the problem Minicourse 1, Toulouse, November 2010

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Theorem We consider a diffeomorphism with a parabolic point of codimension k: f0(z) = z+zk+1 +o(zk+1) For any generic k-parameter unfolding fη, there exists an analytic change of coordinate and parameter (z,η) → (Z,ǫ) in a neighborhood of the origin transforming the family into the prepared form Fǫ(Z) = Z+Pǫ(Z)(1+Qǫ(Z)+Pǫ(Z)K(Z,ǫ))

15 The preparation of the family Minicourse 1, Toulouse, November 2010

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Theorem We consider a diffeomorphism with a parabolic point of codimension k: f0(z) = z+zk+1 +o(zk+1) For any generic k-parameter unfolding fη, there exists an analytic change of coordinate and parameter (z,η) → (Z,ǫ) in a neighborhood of the origin transforming the family into the prepared form Fǫ(Z) = Z+Pǫ(Z)(1+Qǫ(Z)+Pǫ(Z)K(Z,ǫ)) such that, if Z1,...Zk+1 are the fixed points, then F′

ǫ(Zj) = exp

  • P′

ǫ(Zj)

1+a(ǫ)Zk

j

  • 16

The preparation of the family Minicourse 1, Toulouse, November 2010

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This determines almost uniquely the parameters!

The only freedom will be inherited from a rotation of order k in Z Z → τZ; τk = 1 which yields the corresponding change on ǫ:

(ǫk−1,ǫk−2 ...,ǫ0) → (τ2−kǫk−1,τ1−kǫk−2,...,τǫ0)

17 The preparation of the family Minicourse 1, Toulouse, November 2010

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Proof of the theorem We consider a diffeomorphism with a parabolic point of codimension k: f0(z) = z+zk+1 +o(zk+1) A k-parameter unfolding can be written in the form fη(z) = z+pη(z)gη(z), with gη(z) = 1+O(η,z).

18 The preparation of the family Minicourse 1, Toulouse, November 2010

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Using the Weierstrass division theorem on the rest allows to write fη in the form fη(z) = z+pη(z)(1+qη(z)+pη(z)hη(z))

19 The preparation of the family Minicourse 1, Toulouse, November 2010

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Using the Weierstrass division theorem on the rest allows to write fη in the form fη(z) = z+pη(z)(1+qη(z)+pη(z)hη(z)) with pη(z) = zk+1 +νk−1(η)zk−1 +ν1(η)z+ν0(η)

20 The preparation of the family Minicourse 1, Toulouse, November 2010

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Using the Weierstrass division theorem on the rest allows to write fη in the form fη(z) = z+pη(z)(1+qη(z)+pη(z)hη(z)) with pη(z) = zk+1 +νk−1(η)zk−1 +ν1(η)z+ν0(η) and qη(z) = c0(η)+c1(η)z+···+ck(η)zk.

21 The preparation of the family Minicourse 1, Toulouse, November 2010

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Using the Weierstrass division theorem on the rest allows to write fη in the form fη(z) = z+pη(z)(1+qη(z)+pη(z)hη(z)) with pη(z) = zk+1 +νk−1(η)zk−1 +ν1(η)z+ν0(η) and qη(z) = c0(η)+c1(η)z+···+ck(η)zk. Genericity condition: the Jacobian ∂ν ∂η is invertible.

22 The preparation of the family Minicourse 1, Toulouse, November 2010

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Since fη(z) = z+pη(z)(1+qη(z)+pη(z)hη(z)) the fixed points zj of fη are the zeroes of pη.

23 The preparation of the family Minicourse 1, Toulouse, November 2010

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The strategy The formal normal form is the time one map of a vector field Vǫ = Pǫ(Z) 1+a(ǫ)Zk ∂ ∂Z

24 The preparation of the family Minicourse 1, Toulouse, November 2010

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The strategy The formal normal form is the time one map of a vector field Vǫ = Pǫ(Z) 1+a(ǫ)Zk ∂ ∂Z Hence the the fixed points of fη must be sent to the singular points Zj of Vǫ.

25 The preparation of the family Minicourse 1, Toulouse, November 2010

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The strategy The formal normal form is the time one map of a vector field Vǫ = Pǫ(Z) 1+a(ǫ)Zk ∂ ∂Z Hence the the fixed points of fη must be sent to the singular points Zj of Vǫ. Moreover we need have f ′

η(zj) = exp(V ′ ǫ(Zj))

26 The preparation of the family Minicourse 1, Toulouse, November 2010

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How do we find the formal invariant a(ǫ)? Let λj = f ′

η(zj)

We have that

  • 1/ln(λj) = a(ǫ).

27 The preparation of the family Minicourse 1, Toulouse, November 2010

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How do we find the formal invariant a(ǫ)? Let λj = f ′

η(zj)

We have that

  • 1/ln(λj) = a(ǫ).

There exists a polynomial rη(z) of degree ≤ k such that at the points zj we have ln

  • f ′

η(zj)

  • = p′

η(zj)(1+rη(zj)).

28 The preparation of the family Minicourse 1, Toulouse, November 2010

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How do we find the formal invariant a(ǫ)? Let λj = f ′

η(zj)

We have that

  • 1/ln(λj) = a(ǫ).

There exists a polynomial rη(z) of degree ≤ k such that at the points zj we have ln

  • f ′

η(zj)

  • = p′

η(zj)(1+rη(zj)).

(Such a polynomial is found by the Lagrange interpolation formula for distinct zj. The limit exists when two fixed points coallesce (codimension 1 case). We can fill in for the other values of η by Hartogs’s Theorem.)

29 The preparation of the family Minicourse 1, Toulouse, November 2010

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The reparameterization By Kostov theorem, there exists a change of coordinate and parameter transforming the vector field: pη(z)(1+rη(z)) ∂ ∂z = vη(z) into: Pǫ(Z)/(1+a(ǫ)Zk) ∂ ∂Z = Vǫ(Z), where Pǫ(Z) = Zk+1 +ǫk1Zk−1 +ǫ1Z+ǫ0. We apply this change of coordinate and parameter to fη.

30 The preparation of the family Minicourse 1, Toulouse, November 2010

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Claim: this brings fη to a prepared form Fǫ

◮ It sends the zeros zj of pη(z) to the zeroes of

Pǫ(Z). Since the zj are the fixed points of fη, their images are the fixed points Zj of Fǫ.

31 The preparation of the family Minicourse 1, Toulouse, November 2010

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Claim: this brings fη to a prepared form Fǫ

◮ It sends the zeros zj of pη(z) to the zeroes of

Pǫ(Z). Since the zj are the fixed points of fη, their images are the fixed points Zj of Fǫ.

◮ Hence

Fǫ(Z) = Z+Pǫ(Z)Kǫ(Z) = Z+Pǫ(Z)(1+Qǫ(Z)+Pǫ(Z)Hǫ(Z))

32 The preparation of the family Minicourse 1, Toulouse, November 2010

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Claim: this brings fη to a prepared form Fǫ

◮ It sends the zeros zj of pη(z) to the zeroes of

Pǫ(Z). Since the zj are the fixed points of fη, their images are the fixed points Zj of Fǫ.

◮ Hence

Fǫ(Z) = Z+Pǫ(Z)Kǫ(Z) = Z+Pǫ(Z)(1+Qǫ(Z)+Pǫ(Z)Hǫ(Z))

◮ Let be a fixed point. Then

F′

ǫ(Zj) = λj = f ′ η(zj) = exp(v′ η(zj)) = exp(V ′ ǫ(Zj))

which is what we need for a prepared family.

33 The preparation of the family Minicourse 1, Toulouse, November 2010

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The parameters are (almost) canonical We have Fǫ(Z) = Z+Pǫ(Z)Kǫ(Z) = Z+Pǫ(Z)(1+Qǫ(Z)+Pǫ(Z)Hǫ(Z)) Claim: Pǫ, Qǫ and ǫ are unique up to the change Z → τZ; τk = 1 and the corresponding change on ǫ:

(Z,ǫk−1,ǫk−2 ...,ǫ0) → (τZ,τ2−kǫk−1,τ1−kǫk−2,...,τǫ0)

34 The preparation of the family Minicourse 1, Toulouse, November 2010

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The proof Let us suppose that two prepared families fǫ(z) and ˜ f˜

ǫ(˜

z) are conjugate under a map (˜ ǫ, ˜ z) = (h(ǫ),Hǫ(z)): ˜ fh(ǫ) = Hǫ ◦fǫ ◦H−1

ǫ

35 The preparation of the family Minicourse 1, Toulouse, November 2010

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The proof Let us suppose that two prepared families fǫ(z) and ˜ f˜

ǫ(˜

z) are conjugate under a map (˜ ǫ, ˜ z) = (h(ǫ),Hǫ(z)): ˜ fh(ǫ) = Hǫ ◦fǫ ◦H−1

ǫ

fǫ Fixed points zj are those of

vǫ(z) = Pǫ(z)/(1+azk) ∂

∂z

˜ f˜

ǫ

Fixed points ˜ zj are those of

˜ v˜

ǫ(˜

z) = ˜ P˜

ǫ(˜

z)/(1+a˜ zk) ∂

∂˜ z

36 The preparation of the family Minicourse 1, Toulouse, November 2010

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The proof Let us suppose that two prepared families fǫ(z) and ˜ f˜

ǫ(˜

z) are conjugate under a map (˜ ǫ, ˜ z) = (h(ǫ),Hǫ(z)): ˜ fh(ǫ) = Hǫ ◦fǫ ◦H−1

ǫ

fǫ Fixed points zj are those of

vǫ(z) = Pǫ(z)/(1+azk) ∂

∂z

˜ f˜

ǫ

Fixed points ˜ zj are those of

˜ v˜

ǫ(˜

z) = ˜ P˜

ǫ(˜

z)/(1+a˜ zk) ∂

∂˜ z

Note that the formal invariants are the same.

37 The preparation of the family Minicourse 1, Toulouse, November 2010

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Then Hǫ sends the fixed points zj to the fixed points ˜

  • zj. Hence

H∗

ǫ(˜

vh(ǫ))(z) = Pǫ(z)Uǫ(z) ∂ ∂z = wǫ(z) where U = 0.

38 The preparation of the family Minicourse 1, Toulouse, November 2010

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Then Hǫ sends the fixed points zj to the fixed points ˜

  • zj. Hence

H∗

ǫ(˜

vh(ǫ))(z) = Pǫ(z)Uǫ(z) ∂ ∂z = wǫ(z) where U = 0. vǫ and wǫ have the same singular points with same eigenvalues! Hence wǫ = Pǫ(z)

  • 1

1+azk +Pǫ(z)Mǫ(z) ∂ ∂z = vǫ(1+Pǫ(z)Nǫ(z)) ∂ ∂z.

39 The preparation of the family Minicourse 1, Toulouse, November 2010

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There exists Kǫ such that K∗

ǫ(vǫ) = wǫ.

40 The preparation of the family Minicourse 1, Toulouse, November 2010

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There exists Kǫ such that K∗

ǫ(vǫ) = wǫ. Kǫ = ΦTǫ vǫ

is given by the flow of vǫ under the time Tǫ which is solution of vǫ(Tǫ) = − Pǫ(z)Nǫ(z) 1+Pǫ(z)Nǫ(z) which obviously has an analytic solution.

41 The preparation of the family Minicourse 1, Toulouse, November 2010

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There exists Kǫ such that K∗

ǫ(vǫ) = wǫ. Kǫ = ΦTǫ vǫ

is given by the flow of vǫ under the time Tǫ which is solution of vǫ(Tǫ) = − Pǫ(z)Nǫ(z) 1+Pǫ(z)Nǫ(z) which obviously has an analytic solution. Then (K−1

ǫ ◦Hǫ)∗(˜

vh(ǫ)) = vǫ. The result follows from the following theorem proved with L. Teyssier.

42 The preparation of the family Minicourse 1, Toulouse, November 2010

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Theorem (RT) We consider a germ of an analytic change of coordinates Ψ : (z,ǫ) = (z,ǫ0,...,ǫk−1) → (ϕǫ (z),h0 (ǫ),...,hk−1 (ǫ)) = (z,h) at (0,0,··· ,0) ∈ C1+k. The following assertions are equivalent :

  • 1. the families
  • Pǫ(z)

1+a(ǫ)zk ∂ ∂z

  • ǫ and
  • Ph(z)

1+˜ a(h)zk ∂ ∂z

  • h are conjugate

under Ψ,

  • 2. there exist τ with τk = 1 and T(ǫ) an analytic germ such

that, if Rτ(z) = τz

◮ ϕǫ(z) = ΦT(ǫ)

  • Rτ(z)

◮ ǫj = τj−1hj(ǫ), ◮ a(ǫ) = ˜

a(h(ǫ)).

43 The preparation of the family Minicourse 1, Toulouse, November 2010

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Reduction to the case τ = 1 If ϕ′

0(0) = τ we need have τk = 1 in order to

preserve the form of v0.

44 The preparation of the family Minicourse 1, Toulouse, November 2010

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Reduction to the case τ = 1 If ϕ′

0(0) = τ we need have τk = 1 in order to

preserve the form of v0. So we can compose Ψ(z,ǫ) with Rτ and the corresponding change of parameters ǫj = τj−1hj(ǫ) and only discuss the composed family. Hence we can suppose that Ψ(z,ǫ) is such that ϕ′

0(0) = 1.

45 The preparation of the family Minicourse 1, Toulouse, November 2010

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The case ǫ = 0 It is easy to check that the only changes of coordinates tangent to the identity which preserve v0 are the maps Φt

v0.

46 The preparation of the family Minicourse 1, Toulouse, November 2010

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The case ǫ = 0 It is easy to check that the only changes of coordinates tangent to the identity which preserve v0 are the maps Φt

v0.

Indeed, such changes of coordinates have the form z(1+mt(zk)) with mt(z) = tzk +o(zk). The function mt(z) is completely determined by m′

t(0) = t. This is exactly the form of the family

Φt

v0.

47 The preparation of the family Minicourse 1, Toulouse, November 2010

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Reduction to the case ∂k+1ϕǫ

∂zk+1 (0) = 0

We correct ϕ to G(z,t,ǫ) := Φt

vǫ ◦ϕǫ (z)

with t(ǫ) well chosen.

48 The preparation of the family Minicourse 1, Toulouse, November 2010

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Reduction to the case ∂k+1ϕǫ

∂zk+1 (0) = 0

We correct ϕ to G(z,t,ǫ) := Φt

vǫ ◦ϕǫ (z)

with t(ǫ) well chosen. Let H(z,t,ǫ) := ∂k+1G ∂zk+1 (z,t,ǫ) K(t,ǫ) := H(0,t,ǫ) K is analytic and ∂K ∂t (0,0) = (k+1)! = 0.

49 The preparation of the family Minicourse 1, Toulouse, November 2010

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Reduction to the case ∂k+1ϕǫ

∂zk+1 (0) = 0

We correct ϕ to G(z,t,ǫ) := Φt

vǫ ◦ϕǫ (z)

with t(ǫ) well chosen. Let H(z,t,ǫ) := ∂k+1G ∂zk+1 (z,t,ǫ) K(t,ǫ) := H(0,t,ǫ) K is analytic and ∂K ∂t (0,0) = (k+1)! = 0. Let t0 be such that K(t0,0) = 0. By the implicit function theorem, there exists t(ǫ) unique such that t(0) = t0 and K(t(ǫ),ǫ) ≡ 0.

50 The preparation of the family Minicourse 1, Toulouse, November 2010

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Reduction to the case ∂k+1ϕǫ

∂zk+1 (0) = 0

We correct ϕ to G(z,t,ǫ) := Φt

vǫ ◦ϕǫ (z)

with t(ǫ) well chosen. Let H(z,t,ǫ) := ∂k+1G ∂zk+1 (z,t,ǫ) K(t,ǫ) := H(0,t,ǫ) K is analytic and ∂K ∂t (0,0) = (k+1)! = 0. Let t0 be such that K(t0,0) = 0. By the implicit function theorem, there exists t(ǫ) unique such that t(0) = t0 and K(t(ǫ),ǫ) ≡ 0. Composing ϕǫ with Φt(ǫ)

we can suppose that the original family Ψ is such that ∂k+1ϕǫ

∂zk+1 (0) = 0.

51 The preparation of the family Minicourse 1, Toulouse, November 2010

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The rest of the argument is an infinite descent

We introduce the ideal I = ǫ0,...,ǫk−1. We have ϕǫ (z) := z+

  • n≥0

fn (ǫ)zn where fn ∈ I and fk+1 ≡ 0. We must solve

  • 1+a(ǫ)zk

ϕk+1

ǫ

(z)+hk−1ϕk−1

ǫ

(z)+···+h0

  • 1+ ˜

a(h)ϕk

ǫ (z)

  • zk+1 +ǫk−1zk−1 +···+ǫ0
  • ϕ′

ǫ (z) = 0.

It is then clear that hj(ǫ) ∈ I and fj(ǫ) ∈ I.

52 The preparation of the family Minicourse 1, Toulouse, November 2010

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The rest of the argument is an infinite descent

We introduce the ideal I = ǫ0,...,ǫk−1. We have ϕǫ (z) := z+

  • n≥0

fn (ǫ)zn where fn ∈ I and fk+1 ≡ 0. We must solve

  • 1+a(ǫ)zk

ϕk+1

ǫ

(z)+hk−1ϕk−1

ǫ

(z)+···+h0

  • 1+ ˜

a(h)ϕk

ǫ (z)

  • zk+1 +ǫk−1zk−1 +···+ǫ0
  • ϕ′

ǫ (z) = 0.

It is then clear that hj(ǫ) ∈ I and fj(ǫ) ∈ I. Let gjzj be the term of degree j. We will play with the infinite set of equations gj = 0, j ≥ 0.

53 The preparation of the family Minicourse 1, Toulouse, November 2010

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The equations gj = 0 with 0 ≤ j ≤ k−1 yield hj −ǫj ∈ I2, since all other terms in the expression of gj belong to I2.

54 The preparation of the family Minicourse 1, Toulouse, November 2010

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The equations gj = 0 with 0 ≤ j ≤ k−1 yield hj −ǫj ∈ I2, since all other terms in the expression of gj belong to I2. The equation gk+j = 0 with 0 ≤ j ≤ k yields fj ∈ I2.

55 The preparation of the family Minicourse 1, Toulouse, November 2010

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The equations gj = 0 with 0 ≤ j ≤ k−1 yield hj −ǫj ∈ I2, since all other terms in the expression of gj belong to I2. The equation gk+j = 0 with 0 ≤ j ≤ k yields fj ∈ I2. Looking at the linear terms in the equations gℓ = 0 with ℓ > 2k+1 yields fℓ−k ∈ I2. So we have that fj ∈ I2 for all j.

56 The preparation of the family Minicourse 1, Toulouse, November 2010

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The general step by induction

We suppose that hj −ǫj ∈ In when 0 ≤ j ≤ k−1 and fj ∈ In whenever j ≥ 0.

57 The preparation of the family Minicourse 1, Toulouse, November 2010

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The general step by induction

We suppose that hj −ǫj ∈ In when 0 ≤ j ≤ k−1 and fj ∈ In whenever j ≥ 0. To show that hj −ǫj ∈ In+1 for 0 ≤ j ≤ k−1 we consider again the corresponding equations gj = 0, where the only linear terms are hj −ǫj. Hence all other terms of the equation belong to In+1 yielding hj −ǫj ∈ In+1.

58 The preparation of the family Minicourse 1, Toulouse, November 2010

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The general step by induction

We suppose that hj −ǫj ∈ In when 0 ≤ j ≤ k−1 and fj ∈ In whenever j ≥ 0. To show that hj −ǫj ∈ In+1 for 0 ≤ j ≤ k−1 we consider again the corresponding equations gj = 0, where the only linear terms are hj −ǫj. Hence all other terms of the equation belong to In+1 yielding hj −ǫj ∈ In+1. For the same reason the equation gk+j = 0 with 0 ≤ j ≤ k yields fj ∈ In+1 and the equations gℓ = 0 with ℓ > 2k+1 yields fℓ−k ∈ In+1.

59 The preparation of the family Minicourse 1, Toulouse, November 2010