Andrés Navas
U. de Santiago (Chile)
Systèmes dynamiques uniformément et non-
uniformément hyperboliques
Distorted diffeomorphisms and path connectedness of Z^d actions on 1-manifolds
Distorted diffeomorphisms and path connectedness of Z^d actions on 1-manifolds
Distorted diffeomorphisms and path connectedness of Z^d actions on 1-manifolds
Distorted diffeomorphisms and path connectedness of Z^d actions on 1-manifolds
Distorted diffeomorphisms and path connectedness of Z^d actions on 1-manifolds
f → var (log (D f )) (Denjoy...)
V ( f ) := lim
𝑛
𝑣𝑎𝑟 (log 𝐷 𝑓 𝑛)
𝑛
 V (f n) = n V(f )
 V (f) is invariant under conjugacy
• V (f ) = infh{ var(log D(h f h-1))}
For every C2 circle diffeomorphism of irrational rotation number,
the value of V(f ) vanishes (N. 2018).
Remarks:
- This is an analytic consequence of the ergodicity of f (Katok-Herman);
- This implies that such a diffeomorphism approaches the rotation in 1+bv topology by
conjugates (paths of...);
- This result is FALSE for 1+bv diffeomorphisms (Mather non simplicity); the right setting for
the result is the space of diffeomorphisms with absolutely continuous derivative (1+ac).
Vanishing of the asymptotic distortion is equivalent to
• This case reduces to interval diffeomorphisms up to passing to a finite
power (plus some “details”...).
• If a diffeomorphism f has an hyperbolic periodic point, then V ( f )
is automatically positive.
• Let us consider the space D of interval diffeomorphisms with no fixed
point in the interior and parabolic endpoints (Mather, Yoccoz, ...).
V (f ) = var (log DMf )
Here, f belongs to D, and M f denotes its Mather invariant.
• The Mather invariant is a circle diffeomorphism up to pre/post composition
with rotations; it is trivial (i.e. equals the class of rotations) if and only if the
map comes from a C1 vector field;
• The equality above extends to an inequality
| V(f ) - var (log DMf ) | ≤ | log Df (a) | + | log Df (b) |
Distorted diffeomorphisms and path connectedness of Z^d actions on 1-manifolds
• Given a finitely generated group G, an element g is distorted if its
powers gn can be written as products of o(n) factors (generators).
• Given an arbitraty group, an element g is distorted if it is
distorted inside a finitely generated subgroup.
• Question: Given a compact manifold M and r > s, build a Cr diffeomorphism
of M that is Cs distorted yet Cr undistorted.
• Theorem: This exists for r= 2 and M = [a,b]. Moreover, the distortion
achieved is sharp (exponential; Polterovich-Sodin).
Remark. For r=1 this is easier: distorted diffeomorphisms have zero top.
entropy (Calegari-Friedman, Mann, Le Roux, Militon, Rosendal, ...)
• Start with a diffeomorphism f that comes from a vector field.
• Perturb it only on a single fundamental domain: F = fg
• The Mather invariant of F becomes nontrivial, hence F has positive asymptotic
distortion, and therefore is C2 undistorted.
• Do this carefully to ensure C1 distortion...
(N. 2019: using a classical
technique of Kopell, Firmo,
Druck, Bonatti, Farinelli...);
(Dinamarca-Escayola 2020:
using direct computations...).
F = f g
• The sequence of “good” conjugators for a given f is explicit:
• This can be easily transformed into a path of conjugators.
• Moreover, similar formulae work for Zd actions:
• This naturally leads to path-connectedness for Zd actions provided
group elements have zero asymptotic distortion.
The space of Zd actions by C1+ac diffeomorphisms of a 1-manifold is path connected.
Comments:
• Related to an old question by Rosenberg; results by Bonatti-Eynard (connec-tedness,
interval, 𝐶 ∞) and N. (path connectedness, 𝐶 1 ).
 The difficult case is that of the interval with elements having positive asymptotic distortion
though parabolic fixed points.
 There may be infinitely many fixed points; this requires deforming the restriction of the
action to each subinterval with no fixed points in a controlled way.
• If the asymptotic distortion is positive then the Mather invariant is nontrivial, and the centralizer is cyclic
(Mather, Yoccoz...).
• Zd = < f1 , f2 , ... , fd >; there is F such that 𝑓𝑖 = 𝐹 𝑛𝑖
• The naive idea consists in just deforming F (e.g. by linear isotopy) and the action accordingly.
Warning !
It may happen that F is far from the identity
despite each fi is close to it (Sergeraert, Eynard).
Put the action in right coordinates before deforming it:
• Perform the conjugacy trick via the conjugating maps hn
(this is a well-behaved process).
• After this, perform the linear isotopy deformation of the generator h
Fh-1 and deform the action accordingly.
AND MANY THANKS...

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Distorted diffeomorphisms and path connectedness of Z^d actions on 1-manifolds

  • 1. Andrés Navas U. de Santiago (Chile) Systèmes dynamiques uniformément et non- uniformément hyperboliques
  • 7. f → var (log (D f )) (Denjoy...) V ( f ) := lim 𝑛 𝑣𝑎𝑟 (log 𝐷 𝑓 𝑛) 𝑛  V (f n) = n V(f )  V (f) is invariant under conjugacy • V (f ) = infh{ var(log D(h f h-1))}
  • 8. For every C2 circle diffeomorphism of irrational rotation number, the value of V(f ) vanishes (N. 2018). Remarks: - This is an analytic consequence of the ergodicity of f (Katok-Herman); - This implies that such a diffeomorphism approaches the rotation in 1+bv topology by conjugates (paths of...); - This result is FALSE for 1+bv diffeomorphisms (Mather non simplicity); the right setting for the result is the space of diffeomorphisms with absolutely continuous derivative (1+ac).
  • 9. Vanishing of the asymptotic distortion is equivalent to
  • 10. • This case reduces to interval diffeomorphisms up to passing to a finite power (plus some “details”...). • If a diffeomorphism f has an hyperbolic periodic point, then V ( f ) is automatically positive. • Let us consider the space D of interval diffeomorphisms with no fixed point in the interior and parabolic endpoints (Mather, Yoccoz, ...).
  • 11. V (f ) = var (log DMf ) Here, f belongs to D, and M f denotes its Mather invariant. • The Mather invariant is a circle diffeomorphism up to pre/post composition with rotations; it is trivial (i.e. equals the class of rotations) if and only if the map comes from a C1 vector field; • The equality above extends to an inequality | V(f ) - var (log DMf ) | ≤ | log Df (a) | + | log Df (b) |
  • 13. • Given a finitely generated group G, an element g is distorted if its powers gn can be written as products of o(n) factors (generators). • Given an arbitraty group, an element g is distorted if it is distorted inside a finitely generated subgroup.
  • 14. • Question: Given a compact manifold M and r > s, build a Cr diffeomorphism of M that is Cs distorted yet Cr undistorted. • Theorem: This exists for r= 2 and M = [a,b]. Moreover, the distortion achieved is sharp (exponential; Polterovich-Sodin). Remark. For r=1 this is easier: distorted diffeomorphisms have zero top. entropy (Calegari-Friedman, Mann, Le Roux, Militon, Rosendal, ...)
  • 15. • Start with a diffeomorphism f that comes from a vector field. • Perturb it only on a single fundamental domain: F = fg • The Mather invariant of F becomes nontrivial, hence F has positive asymptotic distortion, and therefore is C2 undistorted. • Do this carefully to ensure C1 distortion... (N. 2019: using a classical technique of Kopell, Firmo, Druck, Bonatti, Farinelli...); (Dinamarca-Escayola 2020: using direct computations...). F = f g
  • 16. • The sequence of “good” conjugators for a given f is explicit:
  • 17. • This can be easily transformed into a path of conjugators. • Moreover, similar formulae work for Zd actions: • This naturally leads to path-connectedness for Zd actions provided group elements have zero asymptotic distortion.
  • 18. The space of Zd actions by C1+ac diffeomorphisms of a 1-manifold is path connected. Comments: • Related to an old question by Rosenberg; results by Bonatti-Eynard (connec-tedness, interval, 𝐶 ∞) and N. (path connectedness, 𝐶 1 ).  The difficult case is that of the interval with elements having positive asymptotic distortion though parabolic fixed points.  There may be infinitely many fixed points; this requires deforming the restriction of the action to each subinterval with no fixed points in a controlled way.
  • 19. • If the asymptotic distortion is positive then the Mather invariant is nontrivial, and the centralizer is cyclic (Mather, Yoccoz...). • Zd = < f1 , f2 , ... , fd >; there is F such that 𝑓𝑖 = 𝐹 𝑛𝑖 • The naive idea consists in just deforming F (e.g. by linear isotopy) and the action accordingly. Warning ! It may happen that F is far from the identity despite each fi is close to it (Sergeraert, Eynard).
  • 20. Put the action in right coordinates before deforming it: • Perform the conjugacy trick via the conjugating maps hn (this is a well-behaved process). • After this, perform the linear isotopy deformation of the generator h Fh-1 and deform the action accordingly.