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Generic validity of the multifractal formalism
Aurélia Fraysse
To cite this version:
Aurélia Fraysse. Generic validity of the multifractal formalism. SIAM Journal on Mathematical
Analysis, Society for Industrial and Applied Mathematics, 2007, 39 (2), pp.593-607. �hal-00689978�
Generic validity of the multifractal formalism
A. Fraysse
∗September 13, 2006
Abstract
The multifractal formalism is a conjecture which gives the spectrum of singularities of a signal using numerically computable quantities.
We prove its generic validity by showing that almost every function in a given function space is multifractal and satises the multifractal formalism.
1 Introduction
One motivation of multifractal analysis was the study of fully devel- oped turbulent ows. Indeed, some experimental results obtained in wind-tunnels showed that the regularity of the velocity of a turbulent uid changes wildly from point to point. This quantity is therefore hardly computable. Hence, rather than measure the exponent at some point one rather estimates the fractal dimension of sets where it takes a given value H .
The spectrum of singularities d(H) is the function which gives the Hausdor dimension of those sets. From its denition, it is also almost impossible to obtain numerically the spectrum of singularities.
In [10], two physicists U. Frisch and G. Parisi proposed an al- gorithm in order to derive the spectrum of singularities from quan- tities that are eectively computable on a signal. They proposed to use the L
pmodulus of continuity of the velocity, used in the theory
∗Laboratoire d'analyse et de mathématiques appliquées, Université Paris XII, 61 Avenue du Général de Gaulle, 94010 Créteil Cedex, FRANCE. Email: [email protected]
of turbulent ows since Kolmogorov, [18]. This average quantity is called the scaling function, or scaling exponent and is denoted ξ
f. It is dened by
R|f(x + l) − f (x)|
pdx ∼ |l|
ξf(p), where ∼ means that
R|f (x + l) − f (x)|
pdx is of the order of magnitude of |l|
ξf(p)when l tends to 0 (assuming that the limit exists). Numerical estimations and further results about the scaling function and its wavelet decomposi- tion can be found in [1, 2].
Frisch and Parisi proposed that the spectrum of singularities of a function can be obtained as follows:
d(H) = inf
p∈R
(pH − ξ
f(p) + d), (1) see [10] for the derivation of this formula.
First, we state the mathematical framework of multifractal analy- sis. The main notion we need to dene is the Hölder exponent.
Denition 1. Let α ≥ 0 ; a function f :
Rd→
Ris C
α(x
0) if for all x ∈
Rdsuch that |x − x
0| ≤ 1 there exists a polynomial P of degree less than [α] and a constant C such that,
|f(x) − P (x − x
0)| ≤ C|x − x
0|
α. (2) The Hölder exponent of f at x
0is
h
f(x
0) = sup{α : f ∈ C
α(x
0)}.
It is proved in [14] that for p ≥ 1 , the scaling function ξ
f(p) is closely related with Sobolev or Besov smoothness. It is thus natural for us to replace the scaling function as follows.
If p > 0 η
f(p) = sup{s : f ∈ B
ps/p,∞}. (3) So (1) applied to η
fcan at most give the increasing part of the spec- trum.
Dening, as in [16], an auxiliary function s(1/p) = η(p)/p , the
Besov domain of a function f is the set of (q, t) such that f ∈ B
1/qt,1/q.
The boundary of the Besov domain of f is then given by the graph
of s . And by Sobolev embeddings, the Besov domain of a function
is a convex set. Thus, functions η satisfying (3) are increasing and
concave functions. Furthermore the auxiliary function s is such that
0 ≤ s
0(q) ≤ d . Those conditions lead us to the following denition.
Denition 2. A function η is admissible if s(q) = qη(1/q) is concave and satises 0 ≤ s
0(q) ≤ d . It is strongly admissible if furthermore s(0) > 0 .
The following important result from [16] allows us to dene a metric space using admissible functions.
Proposition 1. Any concave function s satisfying 0 ≤ s
0(q) ≤ d denes the Besov domain of a distribution f .
Thanks to Proposition 1, to each admissible function η , a metric space V can be associated by taking
V =
\ε>0,0<p<∞
B
(η(p)−ε)/p,pp,loc
.
To be as complete as possible, we also recall the denition of Legendre transform.
Denition 3. Let f be a lower semi-continuous function dened in a normed vector space E . Then the Legendre transform of f is
f
∗(x) = sup
y∈E
(f (y) − xy). (4)
This function is convex and lower semi-continuous.
In the present paper, we propose to study the validity of (1) for η
f(p) . An equivalent form of this heuristic formula is satised by a large class of invariant measures, see [4, 6, 20]. In the context of signal analysis, this conjecture is often satised if we add particular assump- tions on f , such as self-similarity. On the other hand, there exist counterexamples to the general validity of this formula. If it does not hold for every function, what is its range of validity? Our purpose here is to show that the validity of formula (1) is not an exceptional phe- nomenon but it is satised for a large class of functions, without any additional assumption. More precisely, we study the validity of this formula for "almost every" functions, i.e. in a measure-theoretic sense.
In a nite dimensional space, the notion of "almost every" means
"for the Lebesgue measure". The particular role played by this mea- sure is justied by the fact that this is the only one which is σ -nite and invariant under translation. In a metric innite dimensional space no measure enjoys this properties. The following denition, see [5, 7, 13]
can thus replace the notion of vanishing Haar measure.
Denition 4. Let V be a complete metric vector space. A Borel set B in V is called Haar null if there exists a probability measure µ with compact support such that
µ(B + v) = 0 ∀v ∈ V. (5)
In this case the measure µ is said transverse to B .
A subset of V is called Haar null if it is contained in a Borel Haar null set.
The complement of a Haar null set is called a prevalent set.
With a slight abuse of language we will say that a property is satised almost everywhere when it holds on a prevalent set.
Let us recall some properties of Haar null sets, see [7, 13].
Proposition 2. 1. If S is Haar-null, then ∀x ∈ V , x + S is Haar- null.
2. If dim(V ) < ∞ , S is Haar-null if and only if meas(S) = 0 (where meas denotes the Lebesgue measure).
3. Prevalent sets are dense.
4. If S is Haar null and S
0⊂ S then S
0is Haar null.
5. The union of a countable collection of Haar null sets is Haar null.
6. If dim(V ) = ∞ , compact subsets of V are Haar-null.
Several kinds of measures can be used as transverse measures of a Borel set. Here, we will only use the following notion.
Denition 5. A nite dimensional space P is called a probe for the set T ⊂ V if the Lebesgue measure on P is transverse to the complement of T .
Those measures are not compactly supported probability mea-
sures. However one immediately checks that Denition 5 is equivalent
to the same one stated with the Lebesgue measure dened on the unit
ball of P . Note that in this case, the support of the measure is included
in the unit ball of a nite dimensional subspace. The compactness as-
sumption is therefore fullled.
The study of generic regularity for a "large" set of functions goes back to S. Banach [3], who gave dierentiability properties of contin- uous functions, for quasi-all functions in the Baire's categories sense.
Later B. Hunt [12] proved the same result in the measure-theoretic sense of prevalence.
In [16], S. Jaard studied properties of generic functions, in the Baire's categories sense, in Sobolev spaces. He also proved that in the sense of Baire's categories quasi-all functions in V satisfy:
d(H) = inf
p≥pc
(pH − η(p) + d) (6)
where p
cis the only critical point such that η(p) = d .
In this paper we will study the validity of the Frisch-Parisi conjec- ture for almost every function in the prevalence setting. The aim of this paper is to prove the following theorem.
Theorem 1. Let η be a strongly admissible function and let V be the space dened by
V =
\ε>0,0<p<∞
B
(η(p)−ε)/p,pp,loc
; (7)
then, in the sense of prevalence, almost every function f in V satises the following two conditions:
1. For all p > 0 ,
η
f(p) = η(p)
2. The spectrum of singularities is dened on the interval
hs(0),
pdc
i
where it is given by:
d
f(H) = inf
p≥pc
(pH − η
f(p) + d) (8) where p
cis the only critical point such that η(p
c) = d .
Remark. We have to impose that η is strongly admissible else, ac- cording to [8], almost every function in V is nowhere locally bounded.
In section 2 we will solve a simpler problem. We will prove that
almost every function in a given intersection of a Sobolev or a Besov
space and an Hölder space satises a slight modication of the Frisch
and Parisi conjecture. We will rst establish their spectrum of singu-
larities.
Theorem 2. If γ > 0 and s −
dp< 0 the spectrum of singularities of almost every function in B
ps,qT
C
γor in L
p,sTC
γis given by:
d(H) =
( d+(γ−s)p
γ
H if H ∈
h
γ,
d+(γ−s)pdγ i−∞ otherwise .
Remarks. 1. Using the Sobolev embeddings B
s,1p, → L
p,s, → B
s,∞p, the same result holds in Sobolev and in Besov spaces. As Besov spaces have a very simple wavelet expansion, we will only prove the result in those spaces. To obtain the Sobolev case, we only need to pick q = ∞ in the following.
2. In Theorem 2 we only state the spectrum of singularities of func- tions in the case B
ps,q∩C
γwhere s−
dp< 0 . Other cases are proved in [9]. To be complete, we recall the following result from [9].
Proposition 3. • If s − d/p ≤ 0 , then almost every function in L
p,sor in B
ps,qis nowhere locally bounded, and therefore its spectrum of singularities is not dened.
• If s − d/p > 0 , then the Hölder exponent of almost every function f of L
p,s, or of B
s,qptakes values in [s − d/p, s] and
∀H ∈ [s − d/p, s] , d
f(H) = Hp − sp + d; (9) furthermore, for almost every x , h
f(x) = s .
Our purpose here is to expand the result of [9] in two directions.
On one hand, we will work with an intersection of Besov spaces.
On the other hand, we will see in the last part another stronger generic result, in the topological sense mentioned above.
The main tool that we will use in the following is the wavelet expansion of functions. First, it yields a simple characterization of functional spaces and it oer a simple condition for pointwise regular- ity. Let us recall some properties of wavelet expansion.
There exist 2
d− 1 oscillating functions (ψ
(i))
i∈{1,...,2d−1}in the Schwartz class such that the functions
2
djψ
(i)(2
jx − k), j ∈
Z, k∈
Zdform an orthonormal basis of L
2(R
d) , see [19]. Wavelets are indexed by dyadic cubes λ = [
2kj;
k+12j[
d. Thus, any function f ∈ L
2can be written:
f (x) =
Xc
(i)j,kψ
(i)(2
jx − k)
where
c
(i)j,k= 2
dj Zf (x)ψ
(i)(2
jx − k)dx.
(Note that we use an L
∞normalization instead of an L
2one, which simplies the formulas). If p > 1 and s > 0 , Sobolev space have thus the following characterization, see [19]:
f ∈ L
p,s⇔
ÃXλ∈Λ
|c
λ|
2(1 + 4
js)χ
λ(x)
!1/2
∈ L
p(R
d), (10) where χ
λ(x) denotes the characteristic function of the cube λ and Λ is the set of all dyadics cubes. Homogeneous Besov spaces, which will also be considered, are characterized (for p, q > 0 and s ∈
R) by
f ∈ B
ps,q⇐⇒
Xj
X
λ∈Λj
|c
λ|
p2
(sp−d)j
q/p
≤ C (11) where Λ
jdenotes the set of dyadics cubes at scale j , see [19]. Note that, if p ∈]0, 1[ , Besov spaces are not Banach spaces since they are not locally convex but nonetheless are separable complete metric vec- tor spaces.
Pointwise regularity can also be expressed in terms of a condition on wavelet coecients, see [14].
Proposition 4. Let x be in
Rd. If f is in C
α(x) then there exists c > 0 such that for all λ :
|c
λ| ≤ c2
−αj(1 + |2
jx − k|)
α. (12)
2 Multifractal formalism in a given Besov space
The Frisch-Parisi conjecture gives the spectrum of singularities as the Legendre transform of the scaling function. We will determine the validity of this formula for measure theoretic generic functions in a given Besov space, in two steps. First we will prove Theorem 2, which one gives the spectrum of singularities of almost every function.
Afterwards, we will give the prevalent scaling function. This allows
us to merge the spectrum obtained with formula (1) applied to the
scaling function.
2.1 Proof of Theorem 2
Proposition 3 states that if s −
dp< 0 , almost every function in B
ps,qis nowhere locally bounded and the spectrum of singularities is not dened for any H . To dene this spectrum, we need to assume a minimum uniform regularity. That is why, in the following, we choose s −
dp< 0 and 0 < γ < s and we study almost every function in B
s,qp∩ C
γ.
Theorem 2.1 from [17], yields an upper bound of the spectrum of singularities.
Lemma 1. Let s −
dp< 0 . For all functions f ∈ B
ps,qTC
γ, the Haus- dor dimension of the set {x : f / ∈ C
α(x)} is bounded by
d+(γ−s)pγα .
We need also the following denition.
Denition 6. Let α ∈ [1,
d+(γ−s)pd] . A point x
0belongs to J
αif there exists an innite sequence (j, k) ∈
N× {0, ..., 2
j− 1}
d, k = (k
1, ..., k
d) such that for each i = 1, ..., d k
ican be written l
i2
j−Land:
1 2
j+
¯¯
¯¯
x
0− k 2
j¯¯
¯¯
< 1
2
αL(13)
where L :=
h(d+(γ−s)p)j d
i
. We dene the exponent of approximation of x as α
0(x) = sup{α : x ∈ J
α} .
In [15], it is proved that the Hausdor dimension of J
αis
dα. Let α ∈
h
1,
d+(γ−s)pd i, ε > 0 and n ∈
Nsuch that N = 2
dn>
εαd+1 be xed. We denote H(α) =
α(d+(γ−s)p)dγand β(α) = H(α) + ε . Each dyadic cube of size 2
−djcan be split into 2
dnsubcubes i(λ) with side 2
−(j+n). We dene the probe P spanned by N functions g
rwith the following wavelet coecients d
rλ:
d
rλ=
(j
−2/q2
−γjif each k
iis a multiple of 2
j−Land r = i(λ)
0 elsewhere (14)
where for each j we denote L =
h(d+(γ−s)p)j d
i
.
One can check that these functions g
rbelong to B
ps,q∩C
γ, see [16].
Let J
α(i, l) =
2li+
£−
2αL1 1 2αL¤d
.
Let us rst check that the set of points S
c(α) dened by S
c(α) = {f =
Xc
λψ
λ∈ B
ps,q∩C
γ: ∃x ∈ J
α∀j, k |c
λ| ≤ c2
−β(α)j(1+|2
jx−k|)
β(α)}.
is a Haar null Borel set. Indeed this set can be included in the lim sup on i of the countable union over l of sets:
S
c(α)
i,l= {f =
Xc
λψ
λ∈ B
s,qp∩C
γ: ∃x ∈ J
α(i, l) ∀j, k |c
λ| ≤ c2
−β(α)j(1+|2
jx−k|)
β(α)}.
which are closed sets.
We pick a sequence of functions f
nin S
c(α)
i,land such that f
ncon- verges to f in B
ps,q∩ C
γ. For each n , there exists x
nin J
α(i, l) such that f
nsatises condition (12) at x
n. But J
α(i, l) is a compact set, so there exists x ∈ J
α(i, l) and a subsequence (x
n(i))
i∈Nsuch that x
n(i)converges to x . As the mapping which gives wavelet coecients of a function is continuous, f satises also (12) at x .
Let f ∈ B
ps,q∩ C
γbe xed. Consider the ane subset M = {δ ∈
RN; f +
Pδ
ig
i∈ S
c(α)} . Let δ
1and δ
2be in M . There exists x
1∈ J
αand x
2∈ J
αsuch that for l = 1, 2 :
|c
λ+
Xδ
ild
iλ| ≤ c2
−β(α)j(1 + |2
jx − k|)
β(α)≤ c2
−αβ(α)L. (15) Furthermore H(α) > γ and, if λ is such that each k is a multiple of 2
j−L.
|d
iλ| > 1
j
2/q2
−H(α)L. (16)
So, taking (15) and (16) we obtain:
kδ
1− δ
2k
RN≤ 2c2
−αβ(α)L2
H(α)Lj
2/q= 2cj
2/q2
−αεL.
When j tends to innity, the Lebesgue measure of S
c(α) tends to zero.
Now, we take the countable union over c and ε
n→ 0 . As Haar null set are stable under inclusion, we obtain:
∀α ∈ [1, d
d + (γ − s)p ] a.e. in B
ps,q∩ C
γ∀x ∈ J
αh
f(x) ≤ H(α).
Let (α
n) be a dense sequence in [1,
d+(γ−s)pd] . As a countable union of Haar null sets is still a Haar null set, for almost every function in B
s,qp∩ C
γ,
h
f(x) ≤ H(α
n) ∀n ∀x ∈ J
αn. (17)
Let f be a function satisfying (17). Let α be xed, there exists a nondecreasing subsequence (α
ϕn) which converges to α and the in- tersection of the subsets J
αϕn(:= ˜ J
α) contains J
α. Furthermore there exist a measure such that any set of dimension less than d/α is of mea- sure zero. And the measure of J
αis positive. If G
H= {x : h
f(x) ≤ H} , with Lemma 1 we have that the Hausdor dimension of G
His
d+(γ−s)p
γ
H . And the
αdHausdor measure of the set {x : h
f(x) < H}
equals zero. This way for almost every function in B
ps,q∩ C
γ, d(H) = d + (γ − s)p
γ H for H ∈
·
γ, dγ
d + (γ − s)p
¸
2.2 The scaling function
Let us now determine the scaling function of almost every function in a given Besov space. We will now show the following result.
Proposition 5. Let s
0and p
0be xed such that s
0−
pd0> 0 . Outside a Haar null set in B
ps00,∞, we have:
η
f(p) =
(ps
0p ≤ p
0d + p(s
0−
pd0
) p ≥ p
0. (18)
Let 0 < γ < s be xed. If s
0−
pd0< 0 , then outside a countable union of compact set in B
sp00,p0TC
γ: η
f(p) =
(
ps
0p ≤ p
0γp + p
0(s
0− γ) p ≥ p
0. (19) Proof : In each case, we can nd in [21] the lower bound. Indeed, this bound is given by the Sobolev embedding.
To prove the upper bound, we will rst consider the case s
0−
pd0
>
0 . Let ε > 0 be xed and denote
˜ s(p) =
(
ps
0+ ε p ≤ p
0d + p(s
0−
pd0
) + ε p ≥ p
0. .
Let 0 < p < ∞ be xed. We want to show that the set of functions
belonging to B
p˜s(p),∞for all 0 < p < ∞ is Haar null. This set is clearly
closed and Borel. Let j ≥ 1 and k ∈ {0, ..., 2
j− 1}
d. We dene J ≤ j and K ∈
Zdsuch that
K 2
J= k
2
jis an irreducible fraction. Let a >
p30
. We dene a probe spanned by the function F with the following wavelet coecients:
d
λ= j
−a2
(pd0−s0)j2
−pd0J. This function belongs to B
ps00,p0.
Let f be in B
ps00,p0and consider the ane subset M = {α ∈
R;f + αF ∈ B
p˜s(p),∞}.
Suppose that there exist α
1and α
2in M . We have then three cases, following position of p .
• If p = p
0, then s(p) = ˜ p
0+ ε and kf + α
1F − (f + α
2F )k
Bs(p),∞˜p
= sup
j
X
k∈{0,...,2j−1}d
| α
1− α
2j
a2
(˜s−pd0)j2
(pd0−s0)j2
−pd0J|
p0= sup
j
| α
1− α
2j
a|2
p0εjXj
J=0
X
K∈{0,...,2J−1}d
2
−dJ= sup
j
|α
1− α
2| j
a2
p0εj. But if α
1and α
2belong to M , this implies that
f + α
1F − (f + α
2F ) belong to B
p˜s(p),∞. This is possible only if α
1= α
2.
• If p > p
0, then s(p) = ˜ d + p(s
0−
pd0
) + ε . In this case, f + α
1F − (f + α
2F ) ∈ B
p˜s(p),∞implies that there exist c > 0 such that:
kf +α
1F −(f +α
2F )k
B˜s(p),∞p
≤ kf +α
1F k
Bs(p),∞˜p
+kf+α
2Fk
B˜s(p),∞p
≤ c.
We have then the following inequalities:
∀j > 0
Xk∈{0,...,2j−1}d
| α
1− α
2j
a2
(˜s−dp)j2
(pd0−s0)j2
−pd0J|
p≤ c
∀j > 0 | α
1− α
2j
a|
p2
(˜s−dp)pj2
(pd0−s0)pj XjJ=0
X
K∈{0,...,2J−1}d
2
−pdp0J≤ c
By denition of J . And
∀j > 0
¯¯
¯¯
α
1− α
2j
a¯¯
¯¯
pXj
J=0
2
(d−dpp0)J≤ c2
(−˜s+dp−pd0+s0)pj∀j > 0
¯¯
¯¯
α
1− α
2j
a¯¯
¯¯
≤ c2
(−˜s+dp−pd0+s0)j¯¯
¯¯
¯
1 1 − 2
j(d−dpp0)¯¯
¯¯
¯
1
p
(20)
As p > p
0, 1 − 2
j(d−dpp0)is equivalent to 1 for large j and (2.2) implies
|α
1− α
2| ≤ cj
a2
−εjwhich tends to zero when j tends to innity.
• If p < p
0, then s(p) = ˜ s
0+ ε and 1 − 2
j(d−dpp0)is equivalent to 2
j(d−dpp0)when j tends to innity. Thus in (2.2), we obtain again
|α
1− α
2| ≤ cj
a2
−εj.
In each case we have obtained that M is of Lebesgue measure zero.
Taking countable union over ε → 0 , and over p , we obtain the desired scaling exponent.
The second case, for s
0−
pd0
< 0 can be treated the same way for p ≤ p
0. The case p > p
0is obtained taking the function which coecients are given by (14) instead of F .
2
From Theorem 2 and Proposition 5, we obtain the following Leg- endre transform of the scaling function of almost every function in a given Besov space.
Proposition 6. Let s
0> 0 and 0 ≤ p
0< ∞ .
• If s
0−
pd0
> 0 , then for almost every function in B
s,qp:
∀H ∈
·
s
0− d
p
0, s
0¸
p>0
inf (d − η(p) + Hp) = d − p
0s
0+ Hp
0. (21)
• If s
0−
pd0< 0 , then for almost every function in B
ps,qTC
γwe have:
∀H ∈ [γ, s
0] inf
p>0
(d − η(p) + Hp) = d − p
0s
0+ Hp
0. (22) This proposition shows that for s
0−
pd0
> 0 , the increasing part of the spectrum given by Frisch-Parisi conjecture is valid for almost every function. But for s
0−
pd0< 0 , this Legendre transform does not correspond to the spectrum of singularities given by Theorem 2.
3 The Frisch-Parisi conjecture
We will now prove Theorem 1. Instead of B
ps00,q0we will now work with:
V =
\ε>0,0<p<∞
B
(η(p)−ε)/p,pp,loc
.
This set V can also be written as a countable intersection over B
(η(ppn,locn)−εn)/pn,pnNote that V is a topological vector space. For p < 1 Besov spaces are only quasi-Banach spaces, as the triangle inequality is only satised up to a constant, V is not a Banach space but a complete metric space.
Indeed, if p ≥ 1 we take for distance between two functions f and g in B
s,qp:
d(f, g) =
Xj≥0
X
k∈{0,...,2j−1}d
¯¯
¯(cj,k
− d
j,k)2
(s−dp)j¯¯
¯p
q p
where c
j,kare the wavelet coecients of f and d
j,kare those of g . If p < 1 Besov spaces are not Banach spaces, but complete metric space with the following distance:
d(f, g) =
X
j≥0
X
k∈{0,...,2j−1}d
|(c
j,k− d
j,k)2
(s−dp)j|
p
q p
min(p,q) q
.
Thus, we obtain a distance in V taking:
∀f, g ∈ V d(f, g) =
Xn
2
−nd
n(f, g) 1 + d
n(f, g)
where d
ndenotes the distance in B
p(η(pn,locn)−εn)/pn,pn. With this distance V is clearly a complete space. Note that the measure used is the Lebesgue measure in the unit ball of a probe, so this is a probability measure with compact support.
In the following subsection we prove that the spectrum of singu- larities of almost every function in V satises:
d(H) = inf
p≥pc
(pH − η(p) + d).
3.1 Proof of Theorem 1
Let us now study the spectrum of singularities on a prevalent set of functions in V .
Proposition 7. For almost every function f ∈ V , the spectrum of singularities satises:
∀H ∈ [s(0), d
p
c] d(H) = inf
p≥pc
(Hp − η(p) + d). (23) Proof :
We will rst construct the probe. Denote:
a(j, k) = inf
p
µ
d(j − J ) − η(p)j
p
¶
and dene g via its wavelet coecients:
d
λ= 1
j
a2
a(j,k)(24)
where we denote a = a
j= log j and J ≤ j is such that there exists K ∈
Zdand
2kj=
2KJis an irreducible form.
First, we check that g belongs to V . Let p > 0 be xed. Thus we have
to show that g ∈ B
η(p)/p,∞p. Let s =
η(p)p. Since a(j, k) ≤
d(j−J)p− sj ,
pa(j, k) + (η(p) − p)j = −Jd and g ∈ B
η(p)/p,∞p. For further details
upon this function g , we refer to [16].
Denition 7. Let α be xed. We denote F
α=
½
x : ∃ a sequence ((k
n, j
n))
n∈N¯¯
¯¯
x − k
n2
jn¯¯
¯¯
≤ 1 2
αjn¾
. (25) The dyadic exponent of x is dened by α(x
0) = sup{α : x
0is α - approximable by dyadics }
As it is stated in [16], the Hausdor dimension of the set F
αis at least
αd.
First, let α ∈ (1, ∞) be xed and let F
αbe the set given by Denition 7. Let ε > 0 be xed, and let
H(α) = 1 α sup
ω≥α
µ
ω sup
q>0
(s(q) − d(1 − 1 ω )q)
¶
and γ = γ(α) = H(α) + ε .
Let n ∈
Nbe such that N = 2
dn>
dε+ 1 be xed. The probe P is spanned by N functions g
iwhich are deduced from g by taking its wavelets coecients only over some sub-cubes i(λ) with size 2
−d(j+n). The aim of this part is to prove that the set of functions f such that there exist a point in F
αwhere f is C
γis a Haar null set. This set is included in the countable union of:
S
c(α) = {f =
Xc
λψ
λ: ∃x ∈ F
α∀j, k |c
λ| ≤ c2
−γ(α)j(1+|2
jx−k|)
γ(α)}.
We can nd a subsequence (j, k) such that J ≤ αj and:
H(α) = 1 α sup
ω≥α
µ
ω sup
q>0
(s(q) − d(1 − 1 ω )q)
¶
≥ −a(j, k).
If x ∈ F
αis xed and λ is such that |x − λ| ≤ A for A > 2N , the wavelet coecients of g
isatisfy:
|d
iλ| ≥ c(A)
j
a2
−H(α)j. (26) We will now prove that the set S
c(α) is a Borel Haar null set.
First, this set is included in the countable union over λ of:
S
c(α)
j,k= {f =
Xc
λψ
λ: ∃x ∈ F
αj,k∀j, k |c
λ| ≤ c2
−γ(α)j(1+|2
jx−k|)
γ(α)}.
Where F
αj,k= {x :
¯¯x −
2kj¯¯≤
21αj} . This set S
c(α)
j,kis a closed set
and S
c(α) is a Borel set. Let f be in V and β
1and β
2be such that
the functions f +
Pβ
1ig
iand f +
Pβ
2ig
iare in S
c(α) . There exist two points x
1and x
2in F
αsuch that in the cone of inuence above x
1and x
2:
|c
λ+
Xβ
1id
iλ− (c
λ+
Xβ
2id
iλ)| ≤ 2c2
−γ(α)j. Or,
|c
λ+
Xβ
i1d
iλ− (c
λ+
Xβ
i2d
iλ)| = |
Xβ
1id
iλ− β
2id
iλ| but, using (26),
|
Xβ
1id
iλ− β
2id
iλ| ≥ |
Xβ
1i− β
2i| c(A)
j
a2
−H(α)j. Thus,
kβ
1− β
2k
RN≤ cj ˜
a2
−εj.
So the Lebesgue measure in
RNof the set {β : f + βg ∈ S
c(α)
j,k} is bounded by (˜ cj
a)
N2
−N εj.
The Lebesgue measure of the set of β such that f +
Pβ
ig
ibelongs to S
c(α) vanishes. Therefore S
c(α) is Haar null.
Taking a countable union over c
n> 0 of sets S
c(α) ,the set of functions in V with a pointwise Hölder exponent greater than γ(α) at a point of F
αis also Haar null. If ε
n→ 0 , taking the union over ε
nit follows that for all α ≥ 1 the set of functions in V with an Hölder exponent greater than H(α) at some point of F
αis Haar null.
Let α
nbe a dense sequence in (1, ∞) . By countable intersection:
M = {f ∈ V : ∀n ∀x ∈ F
αnh
f(x) ≤ H(α)} (27) is prevalent. Let f ∈ M and let α ≥ 1 . There exist a subsequence α
φ(n)which is nondecreasing and tends to α . If we denote F ˜
αthe intersection of sets F
αn, it follows that F ˜
αcontains F
α. Furthermore, the Hausdor dimension of F ˜
αis greater than
αdand for all x ∈ F ˜
α, h
f(x) ≤ H(α) . Finally we obtain
To conclude the second point of Theorem 1 , we rewrite H(α) in the following form
H(α) = 1 α inf
a≥α