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The dynamics of circle maps W. de Melo [email protected] W. de Melo [email protected] () Dynamical Systems , august 2010 1 / 18

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Page 1: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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The dynamics of circle maps

W. de [email protected]

W. de Melo [email protected] () Dynamical Systems , august 2010 1 / 18

Page 2: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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Dynamics in the circle

Circle Diffeomorphismscritical circle mappingscovering maps, expanding circle mapsmultimodal maps

W. de Melo [email protected] () Dynamical Systems , august 2010 2 / 18

Page 3: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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Some problems

Conjugacy classes- conjugacy invariantsFull familiesStructural stability: characterization,densityRigidity: lower regularity of conjugacy⇒higher regularitybifurcation

W. de Melo [email protected] () Dynamical Systems , august 2010 3 / 18

Page 4: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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Poincaré, Denjoy (1932), Arnold (1961),Herman, Yoccoz, .....Yoccoz, (1984), Swiatek (1988), Herman,deMelo-Strien(2000), Yampolski (2002),Khanin-Teplinsky (2007)Shub (1969), Mañe , Shub-SullivandeMelo-Salomão Vargas (2010), Strien,

W. de Melo [email protected] () Dynamical Systems , august 2010 4 / 18

Page 5: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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Lift to the real line

Covering map φ : R→ S1, φ(t) = e2πit

φ(t) = φ(s)⇔ t − s ∈ ZLift of f : S1 → S1:F : R→ R such that φ ◦ F = φ ◦ fF (t + 1) = F (t) + d where d ∈ Ztopological degree of fG another lift of f ⇔ F (t)−G(t) ∈ Z

W. de Melo [email protected] () Dynamical Systems , august 2010 5 / 18

Page 6: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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The standard family: the Arnold´s tongues

Fa,µ(t) = t + a + µ2πsin(2πt)

µ < 1 fa,µ diffeomorphisms, µ = 0 rigidrotationrotation number of a diffeo :ρ(f ) = limn→∞

Fn(x)−xn

µ > 1: rotation interval.

W. de Melo [email protected] () Dynamical Systems , august 2010 6 / 18

Page 7: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

different backgrounds...W. de Melo [email protected] () Dynamical Systems , august 2010 7 / 18

Page 8: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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A dynamical dichotomy

Periodic behavior: x ∈ Pf ⊂ S1 ⇐⇒ ∃neigh. V of x s.t. the orbit of each y ∈ Vis asymptotic to a periodic orbit.Chaotic behavior: Chf = S1 \ Pf

Pf is open and backward invariant. Eachcomponent that does not contain criticalpoint is mapped onto another component.Otherwise is mapped into the closure of acomponent.

W. de Melo [email protected] () Dynamical Systems , august 2010 8 / 18

Page 9: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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Each component of Pf is eventuallymapped in the closure of a periodiccomponent.there is a finite number of periodiccomponents.f diffeomorphism or critical circle map =⇒either Pf is empty and f is top. conj. toirrational rotation or Pf = S1

W. de Melo [email protected] () Dynamical Systems , august 2010 9 / 18

Page 10: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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Full Family

h is a strong semi-conjugacy between fand g if

1 h is continuous, monotone and onto.2 h ◦ f = g ◦ h3 h−1(y) is either a unique point or an interval contained in Pf

A family gµ is 2m-full if any 2m-modal mapf is strongly semi-conjugate to some gµ.The standard family is 2-full(deMelo-Salomão-Vargas: 2m-fulltrigonometric family).

W. de Melo [email protected] () Dynamical Systems , august 2010 10 / 18

Page 11: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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The trigonometric family

fµ : S1 → S1

Fµ : R→ R the lift of fµFµ(t) = dt + µ2m sin(2πmt) +∑m−1

j=0 (µ2j sin(2πjt) + µ2j+1 cos(2πjt))

whereµ = (µ1, . . . , µ2m) ∈ ∆ := {µ ∈ R2m :

µ2m > 0 and fµ is 2m −multimodal }and d ∈ Z, the topological degree of fµ.

W. de Melo [email protected] () Dynamical Systems , august 2010 11 / 18

Page 12: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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Structural Stability and Hyperbolicity

f is hyperbolic if ∃ N s.t |df N(x)| > 1∀x ∈ Chf

Koslovsky-Strien-Shen:structural stability is densef structurally stable⇒ f is hyperbolic

W. de Melo [email protected] () Dynamical Systems , august 2010 12 / 18

Page 13: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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Rigidity- diffeomorphisms

Rigidity: lower regularity of conjugacy implieshigher regularityHerman=Yoccoz: f smooth circle diffeomorphismwhose rotation number is an irrational thatsatisfies a Diophantine condition is smoothlyconjugate to a irrational rotation.Arnold: ∃ smooth diffeo, with irrational rotationnumber (of Liouville type) such that the conjugacywith a rigid rotation maps a set of zero Lebesguemeasure in a set of full Lebesgue measure.

W. de Melo [email protected] () Dynamical Systems , august 2010 13 / 18

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Rigidity of critical circle maps

deMelo-deFaria, Yampolski,Khanin-Templiski, Guarino-deMelo:h C0 conjugacy between two smoothcritical circle maps with irrational rotationnumber⇒ h is C1.

W. de Melo [email protected] () Dynamical Systems , august 2010 14 / 18

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Main tool: renormalization

Critical circle map→ commuting pair ofinterval mapscommuting pair of interval maps→smooth conjugacy class of critical circlemaps.renormalization operator: first return mapto smaller interval around the criticalpoint+ affine rescale

W. de Melo [email protected] () Dynamical Systems , august 2010 15 / 18

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cf(c) f(c)

W. de Melo [email protected] () Dynamical Systems , august 2010 16 / 18

Page 17: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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Complex Bounds

Given an infinitely renormalizablecommuting pair, there exists an integer n0

such that if n.n0 then the n − th iterate ofthe commuting pair by the renormalizationoperator has a holomorphic extension toa holomorphic commuting pair thatbelongs to a compact family.

W. de Melo [email protected] () Dynamical Systems , august 2010 18 / 18

Page 19: W. de Melo demelo@impa - warwick.ac.uk · different backgrounds... The dynamics of circle maps W. de Melo demelo@impa.br W. de Melo demelo@impa.br Dynamical Systems , august 2010

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HOLOMORPHIC PAIR

ηξ (0 )ξ (00)η(

ξ η

ν

a b0 )

W. de Melo [email protected] () Dynamical Systems , august 2010 19 / 18