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Ana Cristina Moreira Freitas CMUP & FEP, Universidade do Porto · 2013. 4. 10. · (CMUP & FEP) 22...

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Extremal index, hitting time statistics and periodicity Ana Cristina Moreira Freitas CMUP & FEP, Universidade do Porto joint work with Jorge Freitas and Mike Todd (CMUP & FEP) 1 / 38
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  • Extremal index, hitting time statistics andperiodicity

    Ana Cristina Moreira FreitasCMUP & FEP, Universidade do Porto

    joint work with Jorge Freitas and Mike Todd

    (CMUP & FEP) 1 / 38

  • Extreme Value Theory

    Consider a stationary stochastic process X0,X1,X2, . . . with marginald.f. F .

    Let F̄ = 1− F and uF = sup{x : F (x) < 1}.

    The main goal of the Extreme Value Theory (EVT) is the study of thedistributional properties of the maximum

    Mn = max{X0, . . . ,Xn−1} (1)

    as n→∞.

    (CMUP & FEP) 2 / 38

  • Extreme Value Laws

    DefinitionWe say that we have an Extreme value law (EVL) for Mn if there is anon-degenerate d.f. H : R→ [0,1] (with H(0) = 0) and for all τ > 0,there exists a sequence of levels un = un(τ) such that

    nP(X0 > un)→ τ as n→∞, (2)

    and for which the following holds:

    P(Mn ≤ un)→ H̄(τ) as n→∞. (3)

    .

    (CMUP & FEP) 3 / 38

  • The independent case

    In the case X0,X1,X2, . . . are i.i.d. r.v. then since

    P(Mn ≤ un) = (F (un))n

    we have that if (2) holds, then (3) holds with H̄(τ) = e−τ :

    P(Mn ≤ un) = (1− P(X0 > un))n ∼(

    1− τn

    )n→ e−τ as n→∞,

    and vice-versa.

    When X0,X1,X2, . . . are not i.i.d. but satisfy some mixing conditionD(un) introduced by Leadbetter then something can still be said aboutH.

    (CMUP & FEP) 4 / 38

  • Condition D(un) from Leadbetter

    Let Fi1,...,indenote the joint d.f. of Xi1 , . . . ,Xin , and setFi1,...,in (u) = Fi1,...,in (u, . . . ,u).

    Condition (D(un))

    We say that D(un) holds for the sequence X0,X1, . . . if for any integersi1 < . . . < ip and j1 < . . . < jk for which j1 − ip > t , and any large n ∈ N,∣∣Fi1,...,ip,j1,...,jk (un)− Fi1,...,ip (un)Fj1,...,jk (un)∣∣ ≤ γ(n, t),where γ(n, tn) −−−→n→∞ 0, for some sequence tn = o(n).

    (CMUP & FEP) 5 / 38

  • Extremal Index

    Theorem (Leadbetter)If D(un) holds for X0,X1, . . . and the limit (3) exists for some τ > 0 thenthere exists 0 ≤ θ ≤ 1 such that H̄(τ) = e−θτ for all τ > 0.

    DefinitionWe say that X0,X1, . . . has an Extremal Index (EI) 0 ≤ θ ≤ 1 if we havean EVL for Mn with H̄(τ) = e−θτ for all τ > 0.

    (CMUP & FEP) 6 / 38

  • Linear normalising sequences

    The sequences of real numbers un = un(τ), n = 1,2, . . ., are usuallytaken to be one parameter linear families such as un = any + bn,where y ∈ R and an > 0, for all n ∈ N.

    Observe that τ depends on y through un and, in fact, depending on thetail of the marginal d.f. F , we have that τ = τ(y) is of one of thefollowing 3 types (for some α > 0):

    Type 1: τ1(y) = e−y for y ∈ R,Type 2: τ2(y) = y−α for y > 0,Type 3: τ3(y) = (−y)α for y ≤ 0.

    (CMUP & FEP) 7 / 38

  • Characterization of the three types

    Theorem (Gnedenko)Necessary and sufficient conditions for τ to be of one of the threetypes are:

    Type 1: There exists some strictly positive function g such that, for allreal y,

    limt↑uF

    1− F (t + yg(t))1− F (t)

    = e−y .

    Type 2: uF =∞ and limt→∞(1− F (ty))/(1− F (t)) = y−α, α > 0, foreach y > 0.

    Type 3: uF 0, for each y > 0.

    (CMUP & FEP) 8 / 38

  • CorollaryThe constants an and bn may be taken as follows:

    Type 1: an = g(γn), bn = γn;

    Type 2: an = γn, bn = 0;

    Type 3: an = uF − γn, bn = uF ,

    where γn = F−1(1− 1/n) = inf{x : F (x) ≥ 1− 1/n}.

    (CMUP & FEP) 9 / 38

  • Examples

    1. If F (x) = 1− e−x then τ is of type 1.

    2. If F (x) = 1− kx−α, α > 0, K > 0, x ≥ K 1/α, then τ is of type 2.

    3. If F (x) = x , 0 ≤ x ≤ 1, then τ is of type 3.

    (CMUP & FEP) 10 / 38

  • Hitting Times and Kac’s Lemma

    Consider the system (X ,B, µ, f ), where X is a topological space, B isthe Borel σ-algebra, f : X → X is a measurable map and µ is anf -invariant probability measure, i.e., µ(f−1(B)) = µ(B), for all B ∈ B.

    For a set A ⊂ X let rA(x) the first hitting time to A of the point x , i.e.rA(x) = min{j ∈ N : f j(x) ∈ A}.

    Let µA denote the conditional measure on A, i.e. µA :=µ|Aµ(A) .

    By Kac’s Lemma, the expected value of rA with respect to µA is∫A

    rA dµA = 1/µ(A).

    (CMUP & FEP) 11 / 38

  • Hitting Time Statistics and Return Time Statistics

    Definition

    Given a sequence of sets (Un)n∈N so that µ(Un)→ 0, the system hasRTS G̃ for (Un)n∈N if for all t ≥ 0

    µUn

    (rUn ≤

    tµ(Un)

    )→ G̃(t) as n→∞. (4)

    and the system has HTS G for (Un)n∈N if for all t ≥ 0

    µ

    (rUn ≤

    tµ(Un)

    )→ G(t) as n→∞, (5)

    For systems with ‘good mixing properties’, G(t) = G̃(t) = 1− e−t , inwhich case we say that we have exponential HTS/RTS.

    (CMUP & FEP) 12 / 38

  • Stationary stochastic processes arising from chaotic dynamics

    Consider a discrete dynamical system

    (X ,B, µ, f ),

    whereX is a d-dimensional Riemannian manifold,B is the Borel σ-algebra,f : X → X is a map,µ is an f -invariant probability measure, absolutely continuous withrespect to Lebesgue (acip).

    (CMUP & FEP) 13 / 38

  • In this context, we consider the stochastic process X0,X1, . . . given by

    Xn = ϕ ◦ f n, for each n ∈ N, (6)

    where ϕ : X → R ∪ {±∞} is an observable (achieving a globalmaximum at ξ ∈ X ) of the form

    ϕ(x) = g(dist(x , ξ)),

    where ξ ∈ X , “dist” denotes a Riemannian metric in X and the functiong : [0,+∞)→ R ∪ {+∞} has a global maximum at 0 and is a strictlydecreasing bijection for a neighborhood V of 0..

    (CMUP & FEP) 14 / 38

  • Observe that if at time j ∈ N we have an exceedance of the level usufficiently large, i.e. Xj(x) > u, then we have an entrance of the orbitof x in the ball of radius g−1(u) around ξ, at time j .

    {X0 > u} = {g(dist(x , ξ)) > u} = {dist(x , ξ) < g−1(u)} = Bg−1(u)(ξ).

    and

    1− F (u) = µ(

    Bg−1(u)(ξ)).

    Based on the characterisation of the 3 types in terms of the tail of F ,we may assume that g is of one of the following 3 types:

    (CMUP & FEP) 15 / 38

  • Type 1: there exists some strictly positive function p : W → R suchthat for all y ∈ R

    lims→g1(0)

    g−11 (s + yp(s))

    g−11 (s)= e−y ; Example: g1(y) = − log y

    Type 2: g2(0) = +∞ and there exists β > 0 such that for all y > 0

    lims→+∞

    g−12 (sy)

    g−12 (s)= y−β; Example: g2(y) = y−1/α

    Type 3: g3(0) = D < +∞ and there exists γ > 0 such that for all y > 0

    lims→0

    g−13 (D − sy)g−13 (D − s)

    = yγ ; Example: g3(y) = D − y1/α

    (CMUP & FEP) 16 / 38

  • Connection between EVL and HTS

    (X ,B, µ, f ) is a dynamical system where µ is an acip.ξ ∈ X are points for which the Lebesgue’s Differentiation Theoremholds.Motivated by Collet’s work, [C01], we obtained:

    Theorem (F,F,Todd (2010))

    If we have HTS G for balls centred on ξ ∈ X , then we have anEVL for Mn with H = G.

    Theorem (F,F,Todd (2010))If we have an EVL H for Mn, then we have HTS G = H for ballscentred on ξ.

    (CMUP & FEP) 17 / 38

  • Idea of the proof:

    {x : Mn(x) ≤ un} =n−1⋂j=0

    {x : Xj(x) ≤ un}

    =n−1⋂j=0

    {x : g(dist(f j(x), ξ)) ≤ un}

    =n−1⋂j=0

    {x : dist(f j(x), ξ) ≥ g−1(un)} = {x : rBg−1(un)(ξ)(x) ≥ n}

    Thus,

    µ{x : Mn(x) ≤ un} = µ{x : rBg−1(un)(ξ)(x) ≥ n}

    (CMUP & FEP) 18 / 38

  • Note that

    τ

    n∼ 1− F (un) = µ

    (Bg−1(un)(ξ)

    )⇔ n ∼ τ

    µ(

    Bg−1(un)(ξ))

    and so

    µ {x : Mn(x) ≤ un} ∼ µ

    x : rBg−1(un)(ξ)(x) ≥ τµ(Bg−1(un)(ξ))→ 1−G(τ)

    (CMUP & FEP) 19 / 38

  • Consider now a sequence δn → 0. We want to study

    µ

    ({x : rBδn (ξ)(x) <

    tµ(Bδn (ξ))

    })Choose `n such that g−1(u`n ) ∼ δn. We have that

    {x : M`n (x) ≤ u`n} =`n−1⋂j=0

    {x : Xj(x) ≤ u`n}

    =`n−1⋂j=0

    {x : g(dist(f j(x), ξ)) ≤ u`n}

    =`n−1⋂j=0

    {x : dist(f j(x), ξ) ≥ g−1(u`n )} = {x : rBg−1(u`n )(ξ)(x) ≥ `n}

    (CMUP & FEP) 20 / 38

  • As before,

    τ

    `n∼ 1− F (u`n ) = µ (Bδn (ξ)) ∼ µ

    (Bg−1(u`n )(ξ)

    )⇔ `n ∼

    τ

    µ (Bδn (ξ)).

    In this way,

    µ

    {x : rBδn (ξ)(x) <

    τ

    µ(Bδn (ξ))

    }∼ 1− µ{x : M`n (x) ≤ u`n} → H(τ)

    (CMUP & FEP) 21 / 38

  • Some history

    EVLs for the partial maximum have been studied in[C01, FF08, FF08a, VHF09, FFT10, FFT11, GHN11, HNT12, FFT12,FFT12a, HVRSB12, FLTV11, FLTV11a, FLTV11b, LFW12, K12,AFV12, FFLTV12].

    The dynamical systems covered in these papers include:

    non-uniformly hyperbolic 1-dimensional maps (in all of them),higher dimensional non-uniformly expanding maps in [FFT10],suspension flows in [HNT12],billiards and Lozi maps in [GHN11]Hénon maps in [FLTV11b, HVRSB12]

    (CMUP & FEP) 22 / 38

  • Incomplete list of papers where a standard exponential HTS/RTS lawhas been proved around almost every point:

    Markov chains in [P91],Axiom A diffeomorphisms in [H93],uniformly expanding maps of the interval in [C96] ,1-dimensional non-uniformly expanding maps in[HSV99, BSTV03, BV03, BT09]...,partially hyperbolic dynamical systems in [D04],toral automorphisms in [DGS04] ,higher dimensional non-uniformly hyperbolic systems (includingHénon maps) in [CC10] .

    (CMUP & FEP) 23 / 38

  • Assuming D(un) holds, let (kn)n∈N be a sequence of integers such that

    kn →∞ and kntn = o(n). (7)

    Condition (D′(un))

    We say that D′(un) holds for the sequence X0,X1, . . . if

    lim supn→∞

    n[n/k ]∑j=1

    P{X0 > un and Xj > un} = 0. (8)

    Theorem (Leadbetter)

    Let {un} be such that n(1− F (un))→ τ , as n→∞, for some τ ≥ 0.Assume that conditions D(un) and D′(un) hold. Then

    P(Mn ≤ un)→ e−τ as n→∞.

    (CMUP & FEP) 24 / 38

  • Assuming D(un) holds, let (kn)n∈N be a sequence of integers such that

    kn →∞ and kntn = o(n). (7)

    Condition (D′(un))

    We say that D′(un) holds for the sequence X0,X1, . . . if

    lim supn→∞

    n[n/k ]∑j=1

    P{X0 > un and Xj > un} = 0. (8)

    Theorem (Leadbetter)

    Let {un} be such that n(1− F (un))→ τ , as n→∞, for some τ ≥ 0.Assume that conditions D(un) and D′(un) hold. Then

    P(Mn ≤ un)→ e−τ as n→∞.

    (CMUP & FEP) 24 / 38

  • Motivated by the work of Collet (2001) we introduced:

    Condition (D2(un))

    We say that D2(un) holds for the sequence X0,X1, . . . if for any integers`, t and n

    |P {X0 > un ∩max{Xt , . . . ,Xt+`−1 ≤ un}}−P{X0 > un}P{M` ≤ un}| ≤ γ(n, t),

    where γ(n, t) is nonincreasing in t for each n and nγ(n, tn)→ 0 asn→∞ for some sequence tn = o(n).

    Theorem (F,F (2008))

    Let {un} be such that n(1− F (un))→ τ , as n→∞, for some τ ≥ 0.Assume that conditions D2(un) and D′(un) hold. Then

    P(Mn ≤ un)→ e−τ as n→∞.

    (CMUP & FEP) 25 / 38

  • Motivated by the work of Collet (2001) we introduced:

    Condition (D2(un))

    We say that D2(un) holds for the sequence X0,X1, . . . if for any integers`, t and n

    |P {X0 > un ∩max{Xt , . . . ,Xt+`−1 ≤ un}}−P{X0 > un}P{M` ≤ un}| ≤ γ(n, t),

    where γ(n, t) is nonincreasing in t for each n and nγ(n, tn)→ 0 asn→∞ for some sequence tn = o(n).

    Theorem (F,F (2008))

    Let {un} be such that n(1− F (un))→ τ , as n→∞, for some τ ≥ 0.Assume that conditions D2(un) and D′(un) hold. Then

    P(Mn ≤ un)→ e−τ as n→∞.

    (CMUP & FEP) 25 / 38

  • Decay of correlations implies D2(un)

    Suppose that there exists a nonincreasing function γ : N→ R suchthat for all φ : X → R with bounded variation and ψ : X → R ∈ L∞,there is C > 0 independent of φ, ψ and n such that∣∣∣∣∫ φ · (ψ ◦ f t )dµ− ∫ φdµ∫ ψdµ∣∣∣∣ ≤ CVar(φ)‖ψ‖∞γ(t), ∀n ≥ 0,

    (9)where Var(φ) denotes the total variation of φ and nγ(tn)→ 0, asn→∞ for some sequence tn = o(n).

    Taking φ = 1{X>un} and ψ = 1{M`≤un}, then

    (9)⇒ D2(un),

    (with γ(n, t) = CVar(1{X>un})‖1{M`≤un}‖∞γ(t) ≤ C′γ(t) and for the

    sequence {tn} such that tn/n→ 0 and nγ(tn)→ 0 as n→∞).(CMUP & FEP) 26 / 38

  • Periodic points

    From here on ξ is a repelling p-periodic point, which implies thatf p(ξ) = ξ, f p is differentiable at ξ and 0 < |det D(f−p)(ξ)| < 1.

    Moreover, we assume ξ ∈ X is a point for which the Lebesgue’sDifferentiation Theorem holds.

    Note that {X0 > u} ∩ {Xp > u} 6= ∅ and for all u sufficiently large

    P({X0 > u} ∩ {Xp > u}) ∼∣∣det D(f−p)(ξ)∣∣P(X0 > u).

    Consequently, D′(un) does not hold since

    n[n/kn]∑j=1

    P(X0 > un,Xj > un) ≥ nP(X0 > un,Xp > un)→∣∣det D(f−p)(ξ)∣∣ τ

    (CMUP & FEP) 27 / 38

  • For repelling periodic points as above, let θ = 1− |det D(f−p)(ξ)|.

    Then the following condition holds:

    Condition (MPp,θ(un))

    We say that X0,X1,X2, . . . satisfies the condition MPp,θ(un) for p ∈ Nand θ ∈ [0,1] if

    limn→∞

    sup1≤j

    un|X0 > un) = 0, limn→∞P(Xp > un|X0 > un) = (1− θ)

    and limn→∞

    supi

    P(Xp > un,X2p > un, . . . ,Xip > un|X0 > un)(1− θ)i

    = 1.

    (CMUP & FEP) 28 / 38

  • Define the event Qp,0(u) := {X0 > u,Xp ≤ u}.

    Observe that for u sufficiently large, Qp,0(u) corresponds to an annuluscentred at ξ.

    Define the events: Qp,i(u) := {Xi > u,Xi+p ≤ u},

    Q∗p,i(u) := {Xi > u} \Qp,i(u) and Qp,s,`(u) =⋂s+`−1

    i=s Qcp,i(u).

    (CMUP & FEP) 29 / 38

  • Theorem (F, F, Todd (2012))

    Let (un)n∈N be such that nP(X0 > un)→ τ , for some τ ≥ 0. SupposeX0,X1, . . . is as in (6) and satisfies MPp,θ(un) for p ∈ N, and θ ∈ (0,1).Then

    limn→∞

    P(Mn ≤ un) = limn→∞P(Qp,0,n(un)) (10)

    First observe that {Mn ≤ un} ⊂ Qp,0,n(un).Moreover, Qp,0,n(un) \ {Mn ≤ un} ⊂

    ⋃n−1i=0 {Xi > un,Xi+p >

    un, . . . ,Xi+si p > un}, where si = [n−1−i

    p ].It follows by MPp,θ(un) and stationarity that

    P(Qp,0,n(un)\{Mn ≤ un}) ≤n−1∑i=0

    P(Xi > un,Xi+p > un, . . . ,Xi+si p > un

    )≤ p

    [n/p]∑i=0

    P(X0 > un,Xp > un,X2p > un, . . . ,Xip > un

    )−−−→n→∞

    0.

    .(CMUP & FEP) 30 / 38

  • Condition (Dp(un))

    We say that Dp(un) holds forX0,X1, . . . if for any `, t and n∣∣P (Qp,0(un) ∩Qp,t ,`(un))− P(Qp,0(un))P(Qp,0,`(un))∣∣ ≤ γ(n, t),where γ(n, t) is nonincreasing in t for each n and nγ(n, tn)→ 0 asn→∞ for some sequence tn = o(n).

    Let (kn)n∈N be a sequence of integers such that kn →∞ andkntn = o(n).

    Condition (D′p(un))

    We say that D′p(un) holds for the sequence X0,X1,X2, . . . if there existsa sequence {kn}n∈N satisfying (7) and such that

    limn→∞

    n[n/kn]∑j=1

    P(Qp,0(un) ∩Qp,j(un)) = 0. (11)

    (CMUP & FEP) 31 / 38

  • Theorem (F, F, Todd (2012))

    Let (un)n∈N be such that nP(X > un)→ τ , as n→∞ for some τ ≥ 0.Consider a stationary stochastic process X0,X1,X2, . . . satisfyingMPp,θ(un) for some p ∈ N, and θ ∈ (0,1). Assume further thatconditions Dp(un) and D′p(un) hold. Then

    limn→∞

    P(Mn ≤ un) = limn→∞P(Qp,0,n(un)) = e−θτ . (12)

    Note that

    P(Qp,0(u)) = P(X0 > u,Xp ≤ u) == P(X0 > u)− P(X0 > u,Xp > u) =∼ P(X0 > u)− (1− θ)P(X0 > u) = θP(X0 > u),

    and so

    θ ∼P(Qp,0(u))P(X0 > u)

    .

    (CMUP & FEP) 32 / 38

  • Applications to specific systems

    Examples of systems for which we can prove the existence of an EI0 < θ < 1 at repelling periodic points

    Systems with decay of correlations against L1 observables:Uniformly expanding maps on the circle ([H93])Conformal repellers and Markov maps ([FP12])Piecewise expanding maps of the interval like Rychlik maps([FFT12, K12])Higher dimensional piecewise expanding maps like in [S00]([FFT12, K12])

    Non-uniformly hyperbolic systems admitting “nice” induced firstreturn time maps:

    Maps with indifferent fixed points like Manneville-Pomeau orLiverani-Saussol-Vaienti maps ([FFT12a])

    Non-uniformly hyperbolic systems with critical points:Benedicks-Carleson quadratic maps ([FFT12a])

    (CMUP & FEP) 33 / 38

  • H. Aytaç, J. M. Freitas, and S. Vaienti, Laws of rare events fordeterministic and random dynamical systems, PreprintarXiv:1207.5188 (2012).

    H. Bruin, B. Saussol, S. Troubetzkoy, and S. Vaienti, Return timestatistics via inducing, Ergodic Theory Dynam. Systems 23 (2003),no. 4, 991–1013.

    H. Bruin and M. Todd, Return time statistics of invariant measuresfor interval maps with positive Lyapunov exponent, Stoch. Dyn. 9(2009), no. 1, 81–100.

    H. Bruin and S. Vaienti, Return time statistics for unimodal maps,Fund. Math. 176 (2003), no. 1, 77–94.

    J.-R. Chazottes and P. Collet, Poisson approximation for thenumber of visits to balls in nonuniformly hyperbolic dynamicalsystems, Preprint arXiv:1007.0171v1 (2010).

    (CMUP & FEP) 33 / 38

  • P. Collet, Some ergodic properties of maps of the interval, inDynamical systems (Temuco, 1991/1992), Travaux en Cours,volume 52, Paris: Hermann (1996), 55–91.

    P. Collet, Statistics of closest return for some non-uniformlyhyperbolic systems, Ergodic Theory Dynam. Systems 21 (2001),no. 2, 401–420.

    M. Denker, M. Gordin, and A. Sharova, A Poisson limit theorem fortoral automorphisms, Illinois J. Math. 48 (2004), no. 1, 1–20.

    D. Dolgopyat, Limit theorems for partially hyperbolic systems,Trans. Amer. Math. Soc. 356 (2004), no. 4, 1637–1689 (electronic).

    D. Faranda, J. M. Freitas, V. Lucarini, G. Turchetti, and S. Vaienti,Extreme value statistics for dynamical systems with noise, PreprintarXiv:1208.5582 (2012).

    (CMUP & FEP) 33 / 38

  • D. Faranda, V. Lucarini, G. Turchetti, and S. Vaienti, Extreme valuedistribution for singular measures, Preprint arXiv:1106.2299v1(2011).

    D. Faranda, V. Lucarini, G. Turchetti, and S. Vaienti, Generalizedextreme value distribution parameters as dynamical indicators ofstability, To appear in Int. J. Bif. Chaos. (arXiv: 1107.5972v1)(2011).

    D. Faranda, V. Lucarini, G. Turchetti, and S. Vaienti, Numericalconvergence of the block-maxima approach to the generalizedextreme value distribution, J. Stat. Phys. 145 (2011), 1156–1180.

    A. Ferguson and M. Pollicott, Escape rates for Gibbs measures,Ergodic Theory Dynam. Systems 32 (2012), no. 3, 961–988.

    A. C. M. Freitas and J. M. Freitas, Extreme values forBenedicks-Carleson quadratic maps, Ergodic Theory Dynam.Systems 28 (2008), no. 4, 1117–1133.

    (CMUP & FEP) 33 / 38

  • A. C. M. Freitas and J. M. Freitas, On the link between dependenceand independence in extreme value theory for dynamical systems,Statist. Probab. Lett. 78 (2008), no. 9, 1088–1093.

    A. C. M. Freitas, J. M. Freitas, and M. Todd, Hitting time statisticsand extreme value theory, Probab. Theory Related Fields 147(2010), no. 3, 675–710.

    A. C. M. Freitas, J. M. Freitas, and M. Todd, Extreme value laws indynamical systems for non-smooth observations, J. Stat. Phys.142 (2011), no. 1, 108–126.

    A. C. M. Freitas, J. M. Freitas, and M. Todd, The compoundPoisson limit ruling periodic extreme behaviour of non-uniformlyhyperbolic dynamics, To appear in Comm. Math. Phys.(arXiv:1204.2304) (2012).

    A. C. M. Freitas, J. M. Freitas, and M. Todd, The extremal index,hitting time statistics and periodicity, Adv. Math. 231 (2012), no. 5,2626 – 2665.

    (CMUP & FEP) 33 / 38

  • C. Gupta, M. Holland, and M. Nicol, Extreme value theory andreturn time statistics for dispersing billiard maps and flows, Lozimaps and Lorenz-like maps, Ergodic Theory Dynam. Systems 31(2011), no. 5, 1363–1390.

    M. Hirata, Poisson law for Axiom A diffeomorphisms, ErgodicTheory Dynam. Systems 13 (1993), no. 3, 533–556.

    M. Hirata, B. Saussol, and S. Vaienti, Statistics of return times: ageneral framework and new applications, Comm. Math. Phys. 206(1999), no. 1, 33–55.

    M. Holland, M. Nicol, and A. Török, Extreme value theory fornon-uniformly expanding dynamical systems, Trans. Amer. Math.Soc. 364 (2012), 661–688.

    M. P. Holland, R. Vitolo, P. Rabassa, A. E. Sterk, and H. W. Broer,Extreme value laws in dynamical systems under physicalobservables, Physica D: Nonlinear Phenomena 241 (2012), no. 5,497 – 513.

    (CMUP & FEP) 33 / 38

  • G. Keller, Rare events, exponential hitting times and extremalindices via spectral perturbation, Dynamical Systems 27 (2012),no. 1, 11–27.

    V. Lucarini, D. Faranda, and J. Wouters, Universal behavior ofextreme value statistics for selected observables of dynamicalsystems, J. Stat. Phys. 147 (2012), no. 1, 63–73.

    B. Pitskel’, Poisson limit law for Markov chains, Ergodic TheoryDynam. Systems 11 (1991), no. 3, 501–513.

    B. Saussol, Absolutely continuous invariant measures formultidimensional expanding maps, Israel J. Math. 116 (2000),223–248.

    R. Vitolo, M. P. Holland, and C. A. T. Ferro, Robust extremes inchaotic deterministic systems, Chaos 19 (2009), no. 4, 043127.

    (CMUP & FEP) 34 / 38

  • Decay of correlations against L1 implies D′p(un)

    Suppose that there exists a nonincreasing function γ : N→ R suchthat for all φ : X → R with bounded variation and ψ : X → R ∈ L1,there is C > 0 independent of φ, ψ and n such that∣∣∣∣∫ φ · (ψ ◦ f t )dµ− ∫ φdµ ∫ ψdµ∣∣∣∣ ≤ CVar(φ)‖ψ‖1γ(t), ∀n ≥ 0,

    (13)where Var(φ) denotes the total variation of φ and nγ(tn)→ 0, asn→∞ for some sequence tn = o(n).

    Taking φ = 1Qp(un) and ψ = 1Qp(un), then

    (13)⇒ D′p(un),

    P(Qp,0(un) ∩Qp,j(un)) ≤ P(Qp,0(un))2 + C′P(Qp,0(un))γ(j) .(τ/n)2 + C′(τ/n)γ(j).

    (CMUP & FEP) 34 / 38

  • Doubling map

    (CMUP & FEP) 35 / 38

  • Rychlik map

    (CMUP & FEP) 36 / 38

  • Intermittent map

    (CMUP & FEP) 37 / 38

  • Benedicks-Carleson maps

    (CMUP & FEP) 38 / 38


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