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A general result on the performance of the wavelet hard thresholding estimator under α-mixing dependence

Christophe Chesneau

To cite this version:

Christophe Chesneau. A general result on the performance of the wavelet hard thresholding estimator underα-mixing dependence. 2014. �hal-00809862v3�

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squared error of the wavelet hard thresholding estimator under α-mixing

dependence

Christophe Chesneau

Laboratoire de Math´ematiques Nicolas Oresme,

Universit´e de Caen BP 5186, F 14032 Caen Cedex, FRANCE. e-mail:

[email protected]

Abstract: In this note, we consider the estimation of an unknown func- tion f for weakly dependent data (α-mixing) in a general setting. Our contribution is theoretical: we prove that a wavelet hard thresholding es- timator attains a sharp rate of convergence under the mean integrated squared error (MISE) over Besov balls without imposing too restrictive as- sumptions on the model. Applications are given for two types of inverse problems: the deconvolution density estimation and the density estimation in a GARCH-type model, both improve existing results in this dependent context. Another application concerns the regression model with random design.

AMS 2000 subject classifications:Primary 62G07, 62G20; secondary 60K35.

Keywords and phrases:Nonparametric statistics,α-mixing dependence, Wavelets, Besov balls, Hard thresholding.

1. Introduction

A general nonparametric problem is adopted: we aim to estimate an unknown functionfvianrandom variablesV1, . . . , Vnfrom a strictly stationary stochastic process (Vt)t∈Z. We suppose that (Vt)t∈Z has a weak dependence structure;

the α-mixing case is considered. This kind of dependence naturally appears in numerous models as Markov chains, GARCH-type models and discretely observed diffusions (see, e.g., Doukhan (1994), Carrasco and Chen (2002) and Bradley (2007)). The problems where f is the density of V1 or a regression function have received a lot of attention. A partial list of related works includes Robinson (1983), Roussas (1987, 1990), Truong and Stone (1992), Tran (1993), Masry (1996a,b), Masry and Fan (1997), Bosq (1998) and Liebscher (2001).

For an efficient estimation off, many methods can be considered. The most popular of them are based on kernels, splines and wavelets. In this note we deal with wavelet methods that have been introduced in i.i.d.setting by Donoho and Johnstone (1994, 1995) and Donoho et al. (1995, 1996). These methods enjoy remarkable local adaptivity against discontinuities and spatially varying degree of oscillations. Complete reviews and discussions on wavelets in statistics can

1

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be found in, e.g., Antoniadis (1997) and H¨ardle et al. (1998). In the context of α-mixing dependence, various wavelet methods have been elaborated for a wide variety of nonparametric problems. Recent developments can be found in, e.g., Leblanc (1996), Tribouley and Viennet (1998), Masry (2000), Patil and Truong (2001), Doosti et al. (2008), Doosti and Niroumand (2009), Doosti et al.

(2010), Cai and Liang (2011), Niu and Liang (2011), Benatia and Yahia (2012), Chesneau (2012, 2013a,b), Chaubey and Shirazi (2014) and Abbaszadeh and Emadi (2013).

In the general dependent setting described above, we provide a theoretical contribution to the performance of a wavelet estimator based on a hard thresh- olding. This nonlinear wavelet procedure has the features to be fully adaptive and efficient over a large class of functionsf (see, e.g., Donoho and Johnstone (1994, 1995), Donoho et al. (1995, 1996) and Delyon and Juditsky (1996)). Fol- lowing the spirit of Kerkyacharian and Picard (2000), we determine necessary assumptions on (Vt)t∈Zand the wavelet basis to ensure that the considered es- timator attains a fast rate of convergence under the MISE over Besov balls.

The obtained rate of convergence often corresponds to the near optimal one in the minimax sense for the standard i.i.d. case. The originality of our result is to be general and sharp; it can be applied for nonparametric models of dif- ferent natures and improves some existing results. This fact is illustrated by the consideration of the density deconvolution estimation problem and the den- sity estimation problem in a GARCH-type model, improving (Chesneau, 2012, Proposition 5.1) and (Chesneau, 2013a, Theorem 2) respectively. A last part is devoted to the regression model with random design. The obtained result completes the one of Patil and Truong (2001).

The organization of this note is as follows. In the next section we describe the considered wavelet setting. The hard thresholding estimator and its rate of convergence under the MISE over Besov balls are presented in Section 3.

Applications of our general result are given in Section 4. The proofs are carried out in Section 5.

2. Wavelets and Besov balls

In this section we introduce some notations corresponding to wavelets and Besov balls.

2.1. Wavelet basis

We consider the wavelet basis on [0,1] constructs from the Daubechies wavelets db2NwithN 1 (see, e.g., Daubechies (1992)). A brief description of this basis is given below. Letφandψbe the initial wavelet functions of the familydb2N.

These functions have the particularity to be compactly supported and to belong to the classCa forN >5a. For any j0, we set Λj ={0, . . . ,2j1} and, for kΛj,

φj,k(x) = 2j/2φ(2jxk), ψj,k(x) = 2j/2ψ(2jxk).

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With appropriated treatments at the boundaries, there exists an integer τ such that, for any integerτ, B={φℓ,k, kΛ; ψj,k; j N− {0, . . . , ℓ 1}, kΛj} is an orthonormal basis ofL2([0,1]), where

L2([0,1]) = (

f : [0,1]R; ||f||2= Z 1

0 |f(x)|2dx 1/2

< )

. For any integerτ andf L2([0,1]), we have the following wavelet expan- sion:

f(x) = X

kΛ

cℓ,kφℓ,k(x) +

X

j=ℓ

X

kΛj

dj,kψj,k(x), x[0,1], wherecj,k anddj,k denotes the wavelet coefficients off defined by

cj,k= Z 1

0

f(x)φj,k(x)dx, dj,k= Z 1

0

f(x)ψj,k(x)dx. (2.1) Technical details can be found in, e.g., Cohen et al. (1993) and Mallat (2009).

In the main result of this paper, we will investigate the MISE rate of the proposed estimator by assuming that the unknown function of interestf belongs to a wide class of functions: the Besov class. Its definition in terms of wavelet coefficients is presented below.

2.2. Besov balls

We say thatf Bp,rs (M) with s >0,p, r1 andM >0 if and only if there exists a constantC > 0 such that the wavelet coefficients of f given by (2.1) satisfy

2τ(1/21/p) X

kΛτ

|cτ,k|p

!1/p

+

X

j=τ

2j(s+1/21/p)

X

kΛj

|dj,k|p

1/p

r

1/r

C,

with the usual modifications ifp=orr=. Note that, for particular choices ofs,pandr,Bsp,r(M) contains the classical H¨older and Sobolev balls (see, e.g., Meyer (1990) and H¨ardle et al. (1998)).

Remark 2.1. We have chosen a wavelet basis on [0,1] to fix the notations;

wavelet basis on another interval can be considered in the rest of the study with- out affecting the results.

3. Statistical framework, estimator and result 3.1. Statistical framework

As mentioned in Section 1, a nonparametric estimation setting as general as possible is adopted: we aim to estimate an unknown functionf L2([0,1]) via

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nrandom variables (or vectors)V1, . . . , Vn from a strictly stationary stochastic process (Vt)t∈Zdefined on a probability space (Ω,A,P). We suppose that (Vt)t∈Z

has a α-mixing dependence structure with exponential decay rate, i.e., there exist two constantsγ >0 andθ >0 such that

sup

m1

eθmαm

γ, where αm = sup(A,B)∈FV

−∞,0×Fm,∞V |P(AB)P(A)P(B)|, F−∞V ,0 is the σ- algebra generated by the random variables (or vectors). . . , V1, V0 and Fm,V

is theσ-algebra generated by the random variables (or vectors) Vm, Vm+1, . . ..

Theα-mixing dependence is reasonably weak; it is satisfied by a wide variety of models including Markov chains, GARCH-type models and discretely ob- served diffusions (see, for instance, Bradley (2007), Carrasco and Chen (2002), Doukhan (1994) and Genon-Catalot et al. (2000)).

The considered estimator forf is presented below.

3.2. Estimator

We define the wavelet hard thresholding estimator ˆf by fˆ(x) = X

kΛj0

ˆ

cj0,kφj0,k(x) +

j1

X

j=j0

X

kΛj

dˆj,k1{|dˆj,k|≥κλj}ψj,k(x), (3.1)

where ˆ cj,k= 1

n

n

X

i=1

q(φj,k, Vi), dˆj,k= 1 n

n

X

i=1

q(ψj,k, Vi), (3.2) 1is the indicator function,κ > 0 is a large enough constant,j0 is the integer satisfying

2j0 = [τlnn], (3.3)

where [a] denotes the integer part ofa,j1 is the integer satisfying 2j1 =

"

n (lnn)3

1/(2ρ+1)#

(3.4)

and

λj = 2ρj rlnn

n . (3.5)

Here it is supposed that there exists a functionq:L2([0,1])×V1(Ω)Csuch that

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(H1) forγ∈ {φ, ψ}, any integerjj0 andkΛj, E(q(γj,k, V1)) =

Z 1 0

f(x)γj,k(x)dx, whereEdenotes the expectation,

(H2) there exist two constants,C >0 andρ0, satisfying, for γ∈ {φ, ψ}, for any integerjj0and kΛj,

(i) supxV1(Ω)|q(γj,k, x)| ≤C2ρj2j/2, (ii) E

|q(γj,k, V1)|2

C22ρj, (iii) for anym∈ {1, . . . , n1},

|Cov(q(γj,k, Vm+1), q(γj,k, V1))| ≤C22ρj2j,

whereCovdenotes the covariance, i.e.,Cov(X, Y) =E(XY)E(X)E(Y), Y denotes the complex conjugate ofY.

For well-known nonparametric models in the i.i.d. setting, wavelet hard thresh- olding estimators and important results can be found in, e.g., Donoho and John- stone (1994, 1995), Donoho et al. (1995, 1996), Delyon and Juditsky (1996), Kerkyacharian and Picard (2000) and Fan and Koo (2002). In the α-mixing context, ˆf defined by (3.1) is a general and improved version of the estimator considered in Chesneau (2012, 2013a). The main differences are the presence of the tuning parameterρ, and the global definition of the function q offering numerous possibilities of applications. Three of them are explored in Section 4.

Comments on the assumptions.The assumption(H1)ensures that (3.2) are unbiased estimators forcj,kanddj,kgiven by (2.1), whereas(H2)is related to their good performance. See Proposition 5.1 below. These assumptions are not too restrictive. For instance, if we consider the standard density estimation problem where (Vt)t∈Zare i.i.d. random variables with bounded densityf, the functionq(γ, x) =γ(x) satisfies(H1) and(H2) withρ= 0 (note that, thanks to the independence of (Vt)t∈Z, the covariance term in(H2)-(iii)is zero). The technical details are given in Donoho et al. (1996).

Lemma 3.1 below describes a simple situation in which the assumption(H2)- (iii)is satisfied.

Lemma 3.1. We make the following assumptions.

(F1) Letube the density ofV1 and,u(V1,Vm+1) be the density of(V1, Vm+1)for any mZ. We suppose that there exists a constantC >0such that

sup

m∈{1,...,n1}

sup

(x,y)V1(Ω)×Vm+1(Ω)|u(V1,Vm+1)(x, y)u(x)u(y)| ≤C.

(F2) There exist two constants, C >0 and ρ0, satisfying, for γ ∈ {φ, ψ}, for any integerjj0 andkΛj,

Z

V1(Ω)|q(γj,k, x)|dxC2ρj2j/2.

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Then, under(F1)and(F2),(H2)-(iii)is satisfied.

3.3. Result

Theorem 3.1 below determines the rate of convergence attained by ˆf under the MISE over Besov balls.

Theorem 3.1. We consider the general statistical setting described in Subsec- tion 3.1. Letfˆbe (3.1)under(H1) and(H2). Suppose thatf Bp,rs (M)with r 1, {p 2 and s (0, N)} or {p [1,2) ands ((2ρ+ 1)/p, N)}. Then there exists a constantC >0 such that

E

kfˆfk22

C lnn

n

2s/(2s+2ρ+1)

. The rate of convergence “((lnn)/n)2s/(2s+2ρ+1)

” is often the near optimal one in the minimax sense for numerous statistical problems in a i.i.d. setting (see, e.g., H¨ardle et al. (1998) and Tsybakov (2004)). Moreover, note that Theorem 3.1 is flexible; the assumptions on (Vt)t∈Z, related to the definition ofqin(H1) and(H2), are mild. In the next section, this flexibility is illustrated for three sophisticated nonparametric estimation problems: the density deconvolution es- timation problem, the density estimation problem in a GARCH-type model and the regression function estimation in the regression model with random design.

4. Applications

4.1. Density deconvolution

Let (Vt)t∈Zbe a strictly stationary stochastic process such that

Vt=Xt+ǫt, tZ, (4.1)

where (Xt)t∈Z is a strictly stationary stochastic process with unknown density f and (ǫt)t∈Z is a strictly stationary stochastic process with known densityg.

It is supposed that ǫt and Xt are independent for anyt Z and (Vt)t∈Z is a α-mixing process with exponential decay rate (see Subsection 3.1 for a precise definition). Our aim is to estimatef viaV1, . . . , Vn from (Vt)t∈Z. Some related works are Masry (1993), Kulik (2008), Comte et al. (2008) and van Zanten and Zareba (2008).

We formulate the following assumptions:

(G1) The support off is [0,1].

(G2) There exists a constantC >0 such that sup

x∈R

f(x)C <.

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(G3) Letube the density ofV1. We suppose that there exists a constantC >0 such that

sup

x∈R

u(x)C.

(G4) For anymZ, let u(V1,Vm+1) be the density of (V1, Vm+1). We suppose that there exists a constantC >0 such that

sup

m∈Z

sup

(x,y)∈R2

u(V1,Vm+1)(x, y)C.

(G5) For any integrable functionγ, we define its Fourier transform by F(γ)(x) =

Z

−∞

γ(y)eixydy, xR.

We suppose that there exist three known constants C > 0, c > 0 and δ >1 such that, for anyxR,

the Fourier transform ofg satisfies

| F(g)(x)| ≥ c (1 +x2)δ/2,

for any∈ {0,1,2}, theℓ-th derivative of the Fourier transform of g satisfies

|(F(g)(x))(ℓ)| ≤ C (1 +|x|)δ+ℓ. We are now in the position to present the result.

Theorem 4.1. We consider the model (4.1). Suppose that(G1)-(G5)are sat- isfied. Letfˆbe defined as in (3.1)with

q(γ, x) = 1

Z

−∞

F(γ)(y)

F(g)(y)eiyxdy, (4.2) whereF(γ)(y)denotes the complex conjugate ofF(γ) (y)andρ=δ(appearing in(G5)).

Suppose that f Bp,rs (M) withr1,{p2 ands(0, N)} or{p[1,2) ands((2δ+ 1)/p, N)}. Then there exists a constant C >0such that

E

kfˆfk22

C lnn

n

2s/(2s+2δ+1)

.

Theorem 4.1 improves (Chesneau, 2012, Proposition 5.1) in terms of rate of convergence; we gain a logaritmic term.

Moreover, it is established that, in the i.i.d. setting, “((lnn)/n)2s/(2s+2δ+1)

is

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exactly the rate of convergence attained by the wavelet hard thresholding estimator,

the near optimal rate of convergence in the minimax sense.

The details can be found in Fan and Koo (2002). Thus Theorem 4.1 can be viewed as an extension of this existing result to the weak dependent case.

4.2. GARCH-type model

We consider the strictly stationary stochastic process (Vt)t∈Z where, for any tZ,

Vt=σt2Zt, (4.3)

t2)t∈Z is a strictly stationary stochastic process with unknown densityf and (Zt)t∈Z is a strictly stationary stochastic process with known density g. It is supposed that σt2 and Zt are independent for any t Z and (Vt)t∈Z is a α- mixing process with exponential decay rate (see Subsection 3.1 for a precise definition). Our aim is to estimatef viaV1, . . . , Vn from (Vt)t∈Z. Some related works are Comte et al. (2008) and Chesneau (2013a).

We formulate the following assumptions:

(J1) There exists a positive integerδsuch that g(x) = 1

1)!(lnx)δ1, x[0,1].

Let us remark that g is the density of Qδ

i=1Ui, where U1, . . . , Uδ are δ i.i.d. random variables having the common distributionU([0,1]).

(J2) The support off is [0,1] andf L2([0,1]).

(J3) Letube the density ofV1. We suppose that there exists a constantC >0 such that

sup

x∈R

u(x)C.

(J4) For any m Z, letu(V1,Vm+1) be the density of (V1, Vm+1). We suppose that there exists a constantC >0 such that

sup

m∈Z

sup

(x,y)∈R2

u(V1,Vm+1)(x, y)C.

We are now in the position to present the result.

Theorem 4.2. We consider the model (4.3). Suppose that(J1)-(J4)are sat- isfied. Letfˆbe defined as in (3.1)with

q(γ, x) =Tδ(γ)(x), (4.4)

where, for any positive integerℓ,T(γ)(x) = (xγ(x))andT(γ)(x) =T(T1(γ))(x) andρ=δ (appearing in(J1)).

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Suppose that f Bp,rs (M) withr1,{p2 ands(0, N)} or{p[1,2) ands((2δ+ 1)/p, N)}. Then there exists a constant C >0such that

E

kfˆfk22

C lnn

n

2s/(2s+2δ+1)

.

Theorem 4.2 significantly improves (Chesneau, 2013a, Theorem 2) in terms of rate of convergence; we gain an exponent 1/2.

4.3. Nonparametric regression model

We consider the strictly stationary stochastic process (Vt)t∈Z where, for any tZ,Vt= (Yt, Xt),

Yt=f(Xt) +ξt, (4.5)

(Xt)t∈Z is a strictly stationary stochastic process with unknown density g, t)t∈Zis a strictly stationary centered stochastic process andf is the unknown regression function. It is supposed thatXtandξtare independent for anytZ and (Vt)t∈Z is aα-mixing process with exponential decay rate (see Subsection 3.1 for a precise definition). Our aim is to estimatefviaV1, . . . , Vnfrom (Vt)t∈Z. Applications of this problem can be foud in H¨ardle (1990). Wavelet methods can be found in Patil and Truong (2001), Doosti et al. (2008), Doosti et al. (2010) and Doosti and Niroumand (2009).

We formulate the following assumptions:

(K1) The support off andg are [0,1] andf and gL2([0,1]).

(K2) ξ1(Ω) is bounded.

(K3) There exists a constantC >0 such that sup

x[0,1]|f(x)| ≤C.

(K4) There exist two constantsc>0 andC >0 such that c inf

x[0,1]g(x), sup

x[0,1]

g(x)C.

(K5) Letube the density ofV1. We suppose that there exists a constantC >0 such that

sup

x∈R×[0,1]

u(x)C.

(K6) For any m Z, letu(V1,Vm+1) be the density of (V1, Vm+1). We suppose that there exists a constantC >0 such that

sup

m∈Z

sup

(x,y)([0,1])×([0,1])

u(V1,Vm+1)(x, y)C.

We are now in the position to present the result.

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Theorem 4.3. We consider the model (4.5). Suppose that(K1)-(K6)are sat- isfied. Letfˆbe the truncated ratio estimator:

fˆ(x) = v(x)ˆ ˆ

g(x)1{|ˆg(x)|≥c/2}, (4.6) where

vˆis defined as in (3.1)with

q(γ,(x, x)) =xγ(x) (4.7) andρ= 0,

gˆis defined as in (3.1)with Xt instead ofVt,

q(γ, x) =γ(x) (4.8)

andρ= 0,

c is the constant defined in (K4).

Suppose that f g Bp,rs (M) and g Bp,rs (M) with r 1, {p 2 and s(0, N)}or{p[1,2)ands(1/p, N)}. Then there exists a constantC >0 such that

E

kfˆfk22

C lnn

n

2s/(2s+1)

.

The estimator (4.6) is derived by combining the procedure of Patil and Truong (2001) with the truncated approach of Vasiliev (2012).

Theorem 4.3 completes Patil and Truong (2001) in terms of rates of conver- gence under the MISE over Besov balls.

Remark 4.1. The assumption(K2)can be relaxed with another strategy to the one developed in Theorem 4.3. Some technical elements are given in Chesneau (2013b).

Conclusion.Considering the weak dependent case on the observations, we prove a general result on the rate of convergence attains by a hard wavelet thresholding estimator under the MISE over Besov balls. This result is flexible;

it can be applied for a wide class of statistical models. Moreover, the obtained rate of convergence is sharp; it can correspond to the near optimal one in the minimax sense for the standard i.i.d. case. Some recent results on sophisticated statistical problems are improved. Thanks to its flexibility, the perspectives of applications of our theoretical result in other contexts are numerous.

5. Proofs

In this section,Cdenotes any constant that does not depend onj,kandn. Its value may change from one term to another and may depend onφorψ.

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5.1. Key lemmas

Let us present two lemmas which will be used in the proofs.

Lemma 5.1 below shows a sharp covariance inequality under the α-mixing condition.

Lemma 5.1 (Davydov (1970)). Let (Wt)t∈Z be a strictly stationary α-mixing process with mixing coefficient αm, m 0, and h and k be two measurable functions. Letp >0 andq >0 satisfying 1/p+ 1/q <1, such thatE(|h(W1)|p) andE(|k(W1)|q)exist. Then there exists a constantC >0 such that

|Cov(h(W1), k(Wm+1))| ≤1m1/p1/q(E(|h(W1)|p))1/p(E(|k(W1)|q))1/q. Lemma 5.2 below presents a concentration inequality forα-mixing processes.

Lemma 5.2 (Liebscher (2001)). Let (Wt)t∈Z be a strictly stationary process with the m-th strongly mixing coefficient αm, m 0, n be a positive integer, h:RCbe a measurable function and, for anytZ,Ut=h(Wt). We assume that E(U1) = 0 and there exists a constant M >0 satisfying |U1| ≤M. Then, for anym∈ {1, . . . ,[n/2]} andλ >0, we have

P 1 n

n

X

i=1

Ui

λ

!

4 exp

λ2n

16(Dm/m+λM m/3)

+ 32M λm,

where

Dm= max

l∈{1,...,2m}

V

l

X

i=1

Ui

! .

5.2. Intermediary results

Proof of Lemma 3.1.Using a standard expression of the covariance, and(F1) and(F2), we obtain

|Cov(q(γj,k, Vm+1), q(γj,k, V1))|

= Z

V1(Ω)

Z

V1(Ω)

q(γj,k, x)q(γj,k, y)(u(V1,Vm+1)(x, y)u(x)u(y))dxdy

Z

V1(Ω)

Z

V1(Ω)|q(γj,k, x)||q(γj,k, y)||u(V1,Vm+1)(x, y)u(x)u(y)|dxdy

C Z

V1(Ω)|q(γj,k, x)|dx

!2

C22ρj2j. This ends the proof of Lemma 3.1.

Proposition 5.1 below proves probability and moments inequalities satisfied by the estimators (3.2).

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Proposition 5.1. Let αˆj,k and βˆj,k be defined as in (3.2) under (H1) and (H2),j0 be (3.3)andj1 be (3.4).

(a) There exists a constant C > 0 such that, for any j ∈ {j0, . . . , j1} and kΛj,

E

|ˆcj,kcj,k|2

C22ρj1 n and

E

dˆj,kdj,k

2

C22ρj1 n.

(b) There exists a constant C > 0 such that, for any j ∈ {j0, . . . , j1} and kΛj,

E

dˆj,kdj,k

4

C24ρj.

(c) Letλj be defined as in (3.5). There exists a constantC >0such that, for any κlarge enough,j∈ {j0, . . . , j1} andkΛj, we have

P

|dˆj,kdj,k| ≥κλj/2

C 1 n4. Proof of Proposition 5.1.

(a) Using(H1)and the stationarity of (Vt)t∈Z, we obtain E |cˆj,kcj,k|2

=Vcj,k)

= 1

n2

n

X

i=1

V(q(φj,k, Vi)) + 2 n2

n

X

v=2 v1

X

ℓ=1

Re(Cov(q(φj,k, Vv), q(φj,k, V)))

= 1

n2

n

X

i=1

V(q(φj,k, Vi)) + 2 n2

n1

X

m=1

(nm)Re(Cov(q(φj,k, Vm+1), q(φj,k, V1)))

1 n E

|q(φj,k, V1)|2 + 2

n1

X

m=1

|Cov(q(φj,k, Vm+1), q(φj,k, V1))|

! .

(5.1) By(H2)-(ii)we get

E

|q(φj,k, V1)|2

C22ρj. (5.2)

For the covariance term, note that

n1

X

m=1

|Cov(q(φj,k, Vm+1), q(φj,k, V1))|=A+B, where

A=

[(lnn)/θ]1

X

m=1

|Cov(q(φj,k, Vm+1), q(φj,k, V1))|

(14)

and

B =

n1

X

m=[(lnn)/θ]

|Cov(q(φj,k, Vm+1), q(φj,k, V1))|. It follows from(H2)-(iii)and 2j2j0<2(lnn)1 that

AC22ρj2j[(lnn)/θ]C22ρj.

The Davydov inequality described in Lemma 5.1 withp=q= 4, (H2)- (i)-(ii)and 2j2j1 ngive

B C

r E

|q(φj,k, V1)|4 nX1

m=[(lnn)/θ]

αm

C2ρj2j/2 r

E

|q(φj,k, V1)|2 X

m=[(lnn)/θ]

eθm/2

= C22ρj

ne(lnn)/2C22ρj. Thus

n1

X

m=1

|Cov(q(φj,k, Vm+1), q(φj,k, V1))| ≤C22ρj. (5.3) Putting (5.1), (5.2) and (5.3) together, the first point in (a) is proved.

The proof of the second point is identical withψinstead ofφ.

(b) Thanks to (H2)-(i), we have |dˆj,k| ≤ supxV1(Ω)|q(ψj,k, x)| ≤ C2ρj2j/2. It follows from the triangular inequality and|dj,k| ≤ ||f||2Cthat

|dˆj,kdj,k| ≤ |dˆj,k|+|dj,k| ≤C2ρj2j/2. This inequality and the second result of(a)yield

E

|dˆj,kdj,k|4

C22ρj2jE

|dˆj,kdj,k|2

C24ρj2j1 n. Using 2j 2j1 n, the proof of(b)is completed.

(c) We will use the Liebscher inequality described in Lemma 5.2. Let us set Ui=q(ψj,k, Vi)E(q(ψj,k, V1)).

We haveE(U1) = 0 and, by(H2)-(i) and 2j 2j1n/(lnn)3,

|Ui| ≤2 sup

xV1(Ω)|q(ψj,k, x)| ≤C2ρj2j/2C2ρj r n

(lnn)3, (soM =C2ρjp

n/(lnn)3).

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