Large deviations principles for lacunary sums Nina Gantert joint - - PowerPoint PPT Presentation
Large deviations principles for lacunary sums Nina Gantert joint - - PowerPoint PPT Presentation
Large deviations principles for lacunary sums Nina Gantert joint work, soon to be finished with Christoph Aistleitner, Zakhar Kabluchko, Joscha Prochno, Kavita Ramanan 1/20 Thanks to: Aicke Hinrichs, Joscha Prochno, Christoph Th ale,
Thanks to: Aicke Hinrichs, Joscha Prochno, Christoph Th¨ ale, Elisabeth Werner for organizing “New Perspectives and Computational Challenges in High Dimensions” MFO, February 2020
2/20
What is a lacunary sum?
First: What is a lacunary sum? Let Ω = [0, 1], P = Lebesgue measure, take an increasing sequence (ak)k∈N of positive integers satifying the Hadamard gap condition ak+1 ak > q for some q > 1. Then, Sn(ω) =
n
- k=1
cos(2πakω) is called lacunary (trigonometric) sum.
3/20
What is a lacunary sum?
Question
Does (Sn) share the properties of a sum of i.i.d. random variables?
Remark
Sn =
n
- k=1
Xk with Xk = cos(2πakω) Xj and Xk are not independent if j = k. X1, X2, . . . are identically distributed Xj and Xk are uncorrelated if j = k.
4/20
Law of large numbers
Law of large numbers:
Theorem (Hermann Weyl)
Sn n → 0 P − a.s. for n → ∞ . (1) Indeed this is true for all ω ∈ [0, 1] \ Q.
Remark
If ak = qk for some q ∈ {2, 3, 4, . . .}, (1) follows from the ergodic theorem: ω = (ω1, ω2, ω3, . . .) where the ωi are i.i.d. and uniform on {0, 1, . . . , q − 1}. qkω mod 1 = T kω where T is the shift transformation: Tω = (ω2, ω3, ω4, . . .). Hence Sn(ω) =
n
- k=1
f (T kω) with f (x) = cos(2πx).
5/20
Law of large numbers
Remark
The last argument is still true if we replace x → cos(2πx) by another 1-periodic function f .
6/20
Central limit theorem
Central limit theorem:
Theorem (Salem, Zygmund)
P
- 1
- n/2
n
- k=1
cos(2πakω) ≤ t
- →
1 √ 2π
t
- −∞
exp
- −u2
2
- du
7/20
Central limit theorem
Question
Does the CLT still hold if we replace x → cos(2πx) by another 1-periodic function f ? Answer: in general, no!
Example (Erd¨
- s, Fortet)
Take f (x) = cos(2πx) + cos(4πx) and ak = 2k − 1, then P
- 1
- n/2
n
- k=1
cos(2πakω) ≤ t
- → F(t)
where F is not the distribution function of a Gaussian law.
8/20
Central limit theorem
Theorem (Kac)
If f is BV and 1
0 f (x)dx = 0 and ak = 2k, the CLT holds with
σ2 =
1
- f (x)2dx + 2
∞
- k=1
1
- f (x)f (2kx)dk .
.
9/20
Law of the iterated logarithm
Law of the iterated logarithm:
Theorem (Erd¨
- s, Gal)
lim sup
n→∞ n
- k=1
cos(2πakω) √n log log n = 1 P -a.s..
10/20
Our question: large deviations?
Our question: large deviations? Let x > 0. Then, P Sn n ≥ x
- → 0 for n → ∞ .
Exponential rate of decay?
11/20
Our question: large deviations?
Theorem
If (ak) obeys the large gap condition ak+1/ak → ∞, then the random variables Sn/n satisfy a large deviation principle with rate function I, where I is given by
- I(x) = − lim
n→∞
1 n log P Sn n ≥ x
- for x > 0, where
Sn =
n
- k=1
cos(2πakUk) with U1, U2, . . . i.i.d. and uniform
- n [0, 1].
Hence, the rate function is the same as for a sum of i.i.d random variables.
- I is convex,
I(1) = I(−1) = +∞.
12/20
Our question: large deviations?
Remark
Sn =
n
- k=1
cos(2πakU1),
- Sn =
n
- k=1
cos(2πakUk) . To show the statement, it suffices to show that for all θ ∈ R lim
n→∞
1 n log E
- eθSn
= lim
n→∞
1 n log E
- eθ
Sn
= Λ(θ) (2) and that θ → Λ(θ) is differentiable.
13/20
Our question: large deviations?
The proof of (2) is simpler in the case when mk := ak+1/ak ∈ N, ∀k. Again, in this case ω can be written as a sequence ω = (ω1, ω2, ω3, . . .) where the ωk are independent, with uniform distribution on {0, 1, . . . , mk − 1}. More precisely, define the filtration F1 ⊂ F2 ⊂ . . ., where Fk+1 := σ
- Jk+1,i, i = 0, . . . , ak+1 − 1
- ,
k ∈ N0, where Jk+1,i :=
- i
ak+1 , i + 1 ak+1
- ,
i = 0, . . . , ak+1 − 1. Let Yk := E [Xk|Fk+1] Then Yk, k ∈ N0 are independent (Yk is a function of ωk!) Xk − Yk∞ ≤ 2π ak ak+1 . (3)
14/20
Our question: large deviations?
Reason for (3): max
ω∈Jk+1,i
|Xk(ω) − Yk(ω)| = max
ω∈Jk+1,i
- Xk(ω) − ak+1
- Jk+1,i
Xk(y) dy
- =
max
ω∈Jk+1,i
- Xk(ω) − Xk(y0)
- ≤
max
ω∈Jk+1,i
2πak
- ω − y0
- ≤ 2π ak
ak+1 , where y0 ∈ Jk+1,i comes from the mean value theorem. Hence, for Sn := n
k=1 Xk and
Sn := n
k=1 Yk,
Sn − Sn∞ ≤ 2π
n
- k=1
ak ak+1 = o(n), n → ∞, because by assumption ak/ak+1 → 0 as k → ∞. This suffices to show (2).
15/20
Our question: large deviations?
Theorem
If ak = qk for some q ∈ {2, 3, 4, . . .}, the random variables Sn/n satisfy a large deviation principle with rate function Iq, Iq = I, Iq(x) → I(x) for q → ∞, for all x ∈ (−1, 1).
16/20
Our question: large deviations?
Theorem
There exists a sequence of positive integers (ak)k∈N satisfying ak+1/ak ≥ q for some q > 1 and all k ∈ N, for which Sn/n does not satisfy a large deviation principle. More precisely, for this sequence (ak)k∈N there exists ¯ x0 ∈ (0, 1) such that for all x0 ∈ (0, ¯ x0), 0 < lim inf
n→∞ −1
n log P(Sn > nx0) < lim sup
n→∞ −1
n log P(Sn > nx0) < ∞.
17/20
Our question: large deviations?
Theorem
There is a sequence (ak) such that ak+1/ak → 2 and the random variables Sn/n satisfy a large deviation principle with rate function I = I2. Hence, large deviations are sensitive to the properties (not only the growth) of the sequence (ak)!
18/20
Our question: large deviations?
Remark (Sublacunary case)
Assume ak → ∞, 1
k log ak → 0, i.e. the Hadamard gap condition is not
- satisfied. Then
1 n log P Sn n ≥ 1 − ε
- → 0 .
Proof There is δ > 0 such that 2πakω ≤ δ ⇒ cos(2πakω) ≥ 1 − ε . But P [2πakω ≤ δ for k ∈ {1, 2, . . . n}] = P [2πanω ≤ δ] = δ 2πan . Hence 1 n log P Sn n ≥ 1 − ε
- ≥ 1
n log δ 2πan → 0 .
19/20
Our question: large deviations?