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Fast-slow systems with chaotic noise Ian Melbourne David Kelly Department of Mathematics University of North Carolina Chapel Hill NC www.dtbkelly.com March 28, 2014 Probability seminar, Universit e Paris Dauphine. Outline Two problems :


  1. Fast-slow systems with chaotic noise Ian Melbourne David Kelly Department of Mathematics University of North Carolina Chapel Hill NC www.dtbkelly.com March 28, 2014 Probability seminar, Universit´ e Paris Dauphine.

  2. Outline Two problems : 1 - Fast-slow systems in continuous time 2 - Fast-slow systems in discrete time

  3. Fast-slow systems in continuous time Let ˙ Y = g ( Y ) be some chaotic ODE with state space Λ and invariant measure µ . We consider fast-slow systems of the form dX ( ε ) = ε − 1 h ( X ( ε ) , Y ( ε ) ) + f ( X ( ε ) , Y ( ε ) ) dt dY ( ε ) = ε − 2 g ( Y ( ε ) ) , dt where ε ≪ 1 and h , f : R e × Λ → R e and � h ( · , y ) µ ( dy ) = 0. Also assume that Y (0) ∼ µ . The aim is to characterize the distribution of X ( ε ) as ε → 0.

  4. Fast-slow systems as SDEs Consider the simplified slow equation dX ( ε ) = ε − 1 h ( X ( ε ) ) v ( Y ( ε ) ) + f ( X ( ε ) ) dt where h : R e → R e × d and v : Λ → R d with � v ( y ) µ ( dy ) = 0. If we write W ( ε ) ( t ) = ε − 1 � t 0 v ( Y ( ε ) ( s )) ds then � t � t X ( ε ) ( t ) = X ( ε ) (0) + h ( X ( ε ) ( s )) dW ( ε ) ( s ) + f ( X ( ε ) ( s )) ds 0 0 where the integral is of Riemann-Lebesgue type.

  5. Invariance principle for W ( ε ) We can write W ( ε ) as ⌊ t /ε 2 ⌋− 1 � t /ε 2 � j +1 W ( ε ) ( t ) = ε � v ( Y ( s )) ds = ε v ( Y ( s )) ds 0 j j =0 The assumptions on Y lead to decay of correlations for the � j +1 sequence v ( Y ( s )) ds . j One can show that W ( ε ) ⇒ W in the sup-norm topology, where W is a multiple of Brownian motion.

  6. What about the SDE? Since � t � t X ( ε ) ( t ) = X ( ε ) (0) + h ( X ( ε ) ( s )) dW ( ε ) ( s ) + f ( X ( ε ) ( s )) ds 0 0 This suggest a limiting SDE � t � t X ( t ) = X (0) + h ( X ( s )) ⋆ dW ( s ) + f ( X ( s )) ds 0 0 But how should we interpret ⋆ dW ?

  7. Continuity with respect to noise (Sussmann ‘78) Suppose that � t � t X ( t ) = X (0) + h ( X ( s )) dU ( s ) + f ( X ( s )) ds , 0 0 where U is a smooth path. If d = 1 or h ( x ) = Id for all x , then Φ : U → X is continuous in the sup-norm topology.

  8. The simple case (Melbourne, Stuart ‘11) If the flow is chaotic enough so that W ( ε ) ⇒ W , and either d = 1 or h = Id then we have that X ( ε ) ⇒ X in the sup-norm topology, where dX = h ( X ) ◦ dW + f ( X ) ds , where the stochastic integral is of Stratonovich type.

  9. This famously falls apart when the noise is both multidimensional and multiplicative . That is, when d > 1 and h � = Id .

  10. Continuity with respect to rough paths (Lyons ‘97) As above, let � t � t X ( t ) = h ( X ( s )) dU ( s ) + F ( X ( s )) ds , 0 0 where U is a smooth path. Let U : [0 , T ] → R d × d be defined by � t U αβ ( t ) def U α ( s ) dU β ( s ) . = 0 Then the map Φ : ( U , U ) �→ X is continuous with respect to the “ ρ γ topology” . We call this the rough path topology .

  11. The rough path topology The ρ γ topology is an extension of the γ -H¨ older topology to the space of objects of the form ( U , U ) ie. the space of rough paths . It has a metric � | U ( s , t ) − V ( s , t ) | + | U ( s , t ) − V ( s , t ) | � ρ γ ( U , U , V , V ) = sup | s − t | γ | s − t | 2 γ s , t ∈ [0 , T ] where � t U βγ ( s , t ) = U β ( s , r ) dU γ ( r ) U ( s , t ) = U ( t ) − U ( s ) and s In particular, it is stronger than the sup-norm topology.

  12. A general theorem for continuous fast-slow systems � t Let W ( ε ) ,αβ ( t ) = 0 W ( ε ) ,α ( s ) dW ( ε ) ,β ( s ). Suppose that ( W ( ε ) , W ( ε ) ) ⇒ ( W , W ) in the sup-norm topology where W is Brownian motion and � t W αβ ( t ) = W α ( s ) ◦ dW β ( s ) + λ αβ t 0 where λ ∈ R d × d and that ( W ( ε ) , W ( ε ) ) satisfy the tightness estimates . Then X ( ε ) ⇒ X in the sup norm topology, where   � λ ik ∂ j h i ( X ) h k  dt dX = h ( X ) ◦ dW +  f ( X ) + j ( X ) i , j , k

  13. Tightness estimates To lift a sup-norm invariance principle to a ρ γ invariance principle, we use the Kolmogorov criterion . Let W ( ε ) ( s , t ) = W ( ε ) ( t ) − W ( ε ) ( s ) � t W ( ε ) ,αβ ( s , t ) = W ( ε ) ,α ( s , r ) dW ( ε ) ,β ( r ) s The tightness estimates are of the form ( E µ | W ( ε ) ( s , t ) | q ) 1 / q � | t − s | α and ( E µ | W ( ε ) ( s , t ) | q / 2 ) 2 / q � | t − s | 2 α for q large enough and α > 1 / 3.

  14. We have the following result Theorem (K, Melbourne ‘14) If the fast dynamics are ”sufficiently chaotic”, then ( W ( ε ) , W ( ε ) ) ⇒ ( W , W ) where W is a Brownian motion and � t W α ( s ) ◦ dW β ( s ) + 1 W αβ ( t ) = 2 λ αβ t 0 where � ∞ λ βγ = E µ ( v β v γ ( Y ( s )) − v β ( Y ( s )) v γ ) ds . 0

  15. Homogenized equations Corollary Under the same assumptions as above, the slow dynamics X ( ε ) ⇒ X where   � λ ik ∂ j h i ( X ) h k  dt . dX = h ( X ) ◦ dW +  f ( X ) + j ( X ) i , j , k Rmk. The only case where one gets Stratonovich is when the Auto-correlation is symmetric. For instance, if the flow is reversible .

  16. Now let’s try discrete time ...

  17. Discrete time fast-slow systems Suppose that T : Λ → Λ is a chaotic map with invariant measure µ . We consider the discrete fast-slow system X ( n ) j +1 = X ( n ) + n − 1 / 2 h ( X ( n ) , T j ) + n − 1 f ( X ( n ) , T j ) j j j Now define the path X ( n ) ( t ) = X ( n ) ⌊ nt ⌋ . The aim is to characterize the distribution of the path X ( n ) as n → ∞ .

  18. Fast-slow systems as SDEs Lets again simplify the slow equation to X ( n ) j +1 = X ( n ) + n − 1 / 2 h ( X ( n ) ) v ( T j ) . j j If we sum these up, we get ⌊ nt ⌋− 1 ) v ( T j ) h ( X ( n ) X ( n ) ( t ) = X ( n ) (0) + � j n 1 / 2 j =0 If we write W ( n ) ( t ) = n − 1 / 2 � ⌊ nt ⌋− 1 v ( T j ) then the path X ( n ) ( t ) j =0 satisfies � t X ( n ) ( t ) = X (0) + h ( X ( n ) ( s − )) dW ( n ) ( s ) 0 where the integral is defined in the “left-Riemann sum” sense.

  19. Invariance principle ⌊ nt ⌋− 1 � W ( n ) ( t ) = n − 1 / 2 v ( T j ) j =0 We still have that W ( n ) ⇒ W in the Skorokhod topology, where W is a multiple of Brownian motion. But W ( n ) is a step function ... so RPT doesn’t really work... even if it did, you’ll never satisfy the tightness estimates.

  20. A general theorem for discrete fast-slow systems (K 14’) Let W ( n ) ,αβ ( t ) = n − 1 � v α ( T i ) v β ( T j ) 0 ≤ i < j < ⌊ nt ⌋ Suppose that ( W ( n ) , W ( n ) ) ⇒ ( W , W ) in the Skorokhod topology where W is Brownian motion and � t W αβ ( t ) = W α ( s ) ◦ dW β ( s ) + λ αβ t 0 where λ ∈ R d × d and that ( W ( n ) , W ( n ) ) satisfy the discrete tightness estimates . Then X ( n ) ⇒ X in the Skorokhod topology, where � λ ik ∂ j h i ( X ) h k dX ( t ) = h ( X ) ◦ dW + j ( X ) dt i , j , k

  21. Discrete tightness estimates The discrete tightness estimates are a courser version of the Kolmogorov criterion. Let W ( n ) ,α ( s , t ) = n − 1 / 2 � v α ( T i ) ⌊ ns ⌋≤ i < ⌊ nt ⌋ W ( n ) ,αβ ( s , t ) = n − 1 � v α ( T i ) v β ( T j ) ⌊ ns ⌋≤ i < j < ⌊ nt ⌋ Then the discrete tightness estimates are of the form α � � ( E µ | W ( n ) ( j n , k j − k n ) | q ) 1 / q � � � and � � n � � 2 α � � ( E µ | W ( n ) ( j n , k j − k n ) | q / 2 ) 2 / q � � � � � n � � for all j , k = 0 , . . . , n , for q large enough and α > 1 / 3.

  22. We have the following result Theorem (K, Melbourne ‘14) If the fast dynamics are ”sufficiently chaotic”, then ( W ( n ) , W ( n ) ) ⇒ ( W , W ) in the Skorokhod topology, where W is a Brownian motion and � t W α ( s ) ◦ dW β ( s ) + 1 W αβ ( t ) = 2 κ αβ t 0 where ∞ κ αβ = � E µ v α v β ( T j ) j =1

  23. Homogenized equations Corollary Under the same assumptions as above, the slow dynamics X ( n ) ⇒ X where 1 � 2 κ jk ∂ i h j ( X ) h ik ( X ) dt . dX = h ( X ) ◦ dW + i , j , k

  24. Idea of proof Recall that X ( n ) j +1 = X ( n ) + n − 1 / 2 h ( X ( n ) ) v ( T j ) . j j The idea is to approximate X ( n ) ( t ) = X ( n ) ⌊ nt ⌋ by ˜ X ( n ) ( t ), which solves an equation driven by smooth paths.

  25. Idea of proof This can be achieved by finding a (piecewise smooth) rough path W ( n ) = ( ˜ ˜ W ( n ) , ˜ W ( n ) ) such that � � � � W ( n ) ( j W ( n ) ( j W ( n ) ( j n ) , W ( n ) ( j ˜ n ) , ˜ n ) = n ) for all j = 0 , . . . , n and which is Lipschitz in between mesh points. Then define � t X ( n ) ( t ) = X (0) + ˜ h ( ˜ X ( n ) ( s )) d ˜ W ( n ) ( s ) 0

  26. Idea of proof Alternatively we can write � t X ( n ) ( t ) = X (0) + ˜ h ( ˜ X ( n ) ( s )) d ˜ W ( n ) ( s ) 0 � t 1 � 2 ∂ i h j ( X ) h ik ( X ) dZ ( n ) , jk ( s ) + 0 i , j , k where Z ( n ) is a piecewise smooth path.

  27. Idea of proof X ( n ) is a good approximation of X ( n ) . By construction, ˜ Proposition We have that X ( n ) ( j / n ) | � K n ,γ n 1 − 3 γ , | X ( n ) ( j / n ) − ˜ sup j =0 ... n for any γ ∈ (1 / 3 , 1 / 2] , where the constant K n ,γ depends on n older norms” of ( W ( n ) , W ( n ) ) . through the “discrete H¨ X ( n ) ⇒ X then X ( n ) ⇒ X . As a consequence, if ˜

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