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Introduction Persistence Probability Ideas from the Proofs Persistence of Gaussian stationary processes Naomi D. Feldheim Joint work with Ohad N. Feldheim Department of Mathematics Tel-Aviv University Darmstadt July, 2014

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Page 1: Introduction Persistence Probability Ideas from the Proofsohadfeld/Papers/Long gaps for... · Introduction Persistence Probability Ideas from the Proofs Definitions Examples General

IntroductionPersistence ProbabilityIdeas from the Proofs

Persistence of Gaussian stationary processes

Naomi D. FeldheimJoint work with Ohad N. Feldheim

Department of MathematicsTel-Aviv University

DarmstadtJuly, 2014

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DefinitionsExamplesGeneral Construction

Real Gaussian Stationary Processes (GSP)

Let T ∈ {Z,R}. A GSP is a random function f : T → R s.t.

It has Gaussian marginals:∀n ∈ N, x1, . . . , xn ∈ T : (f (x1), . . . , f (xn)) ∼ NRn(0,Σ)

It is Stationary:∀n ∈ N, x1, . . . , xn ∈ T and ∀t ∈ T :(f (x1 + t), . . . , f (xn + t)

) d∼(f (x1), . . . , f (xn)

)

If T = Z we call it a GSS (Gaussian Stationary Sequence).If T = R we call it a GSF (Gaussian Stationary Function). Weassume GSFs are a.s. continuous.

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Covariance kernel

For a GSP f : T → R the covariance kernel r : T → R is definedby:

r(x) = E [f (0)f (x)] = E [f (t)f (x + t)] .

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DefinitionsExamplesGeneral Construction

Covariance kernel

For a GSP f : T → R the covariance kernel r : T → R is definedby:

r(x) = E [f (0)f (x)] = E [f (t)f (x + t)] .

determines the process f .

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DefinitionsExamplesGeneral Construction

Covariance kernel

For a GSP f : T → R the covariance kernel r : T → R is definedby:

r(x) = E [f (0)f (x)] = E [f (t)f (x + t)] .

determines the process f .

positive-definite:∑

1≤i ,j≤n cicj r(xi − xj) ≥ 0.

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DefinitionsExamplesGeneral Construction

Covariance kernel

For a GSP f : T → R the covariance kernel r : T → R is definedby:

r(x) = E [f (0)f (x)] = E [f (t)f (x + t)] .

determines the process f .

positive-definite:∑

1≤i ,j≤n cicj r(xi − xj) ≥ 0.

symmetric: r(−x) = r(x).

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DefinitionsExamplesGeneral Construction

Covariance kernel

For a GSP f : T → R the covariance kernel r : T → R is definedby:

r(x) = E [f (0)f (x)] = E [f (t)f (x + t)] .

determines the process f .

positive-definite:∑

1≤i ,j≤n cicj r(xi − xj) ≥ 0.

symmetric: r(−x) = r(x).

continuous.

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Spectral measure

Bochner’s Theorem

Write Z∗ = [−π, π], R∗ = R. Then

r(x) = ρ̂(x) =

T∗

e−ixλdρ(λ),

where ρ is a finite, symmetric, non-negative measure on T ∗.

We call ρ the spectral measure of f .

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Spectral measure

Bochner’s Theorem

Write Z∗ = [−π, π], R∗ = R. Then

r(x) = ρ̂(x) =

T∗

e−ixλdρ(λ),

where ρ is a finite, symmetric, non-negative measure on T ∗.

We call ρ the spectral measure of f .We assume:

∃δ > 0 :

∫|λ|δdρ(δ) <∞.

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Toy-Example Ia - Gaussian wave

ζj i.i.d. N (0, 1)f (x) = ζ0 sin(x) + ζ1 cos(x)r(x) = cos(x)ρ = 1

2 (δ1 + δ−1)

0 1 2 3 4 5 6 7 8 9 10−1

−0.8

−0.6

−0.4

−0.2

0

0.2

0.4

0.6

0.8

1

Three Sample Paths

−10 −5 0 5 10−1

−0.8

−0.6

−0.4

−0.2

0

0.2

0.4

0.6

0.8

1

Covariance Kernel

−2 −1.5 −1 −0.5 0 0.5 1 1.5 20

0.05

0.1

0.15

0.2

0.25

0.3

0.35

0.4

0.45

0.5

Spectral Measure

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Toy-Example Ib - Almost periodic wave

f (x) =ζ0 sin(x) + ζ1 cos(x)

+ ζ2 sin(√2x) + ζ3 cos(

√2x)

r(x) = cos(x) + cos(√2x)

ρ = 12

(δ1 + δ−1 + δ√2 + δ−

√2

)

0 1 2 3 4 5 6 7 8 9 10−2.5

−2

−1.5

−1

−0.5

0

0.5

1

1.5

2

2.5

Three Sample Paths−10 −8 −6 −4 −2 0 2 4 6 8 10−1

−0.8

−0.6

−0.4

−0.2

0

0.2

0.4

0.6

0.8

1

Covariance Kernel

−2 −1.5 −1 −0.5 0 0.5 1 1.5 20

0.05

0.1

0.15

0.2

0.25

0.3

0.35

0.4

0.45

0.5

Spectral Measure

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Example II - i.i.d. sequence

f (n) = ζnr(n) = δn,0dρ(λ) = 1

2π1I[−π,π](λ)dλ

0 1 2 3 4 5 6 7 8 9 10−1.5

−1

−0.5

0

0.5

1

1.5

2

Three Sample Paths

−5 −4 −3 −2 −1 0 1 2 3 4 5−1

−0.8

−0.6

−0.4

−0.2

0

0.2

0.4

0.6

0.8

1

Covariance Kernel

−5 −4 −3 −2 −1 0 1 2 3 4 50

0.02

0.04

0.06

0.08

0.1

0.12

0.14

0.16

0.18

0.2

Spectral Measure

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Example IIb - Sinc Kernel

f (x) =∑

n∈N ζn sinc(x − n)

r(x) = sin(πx)πx = sinc(x)

dρ(λ) = 12π1I[−π,π](λ)dλ

0 1 2 3 4 5 6 7 8 9 10−1.5

−1

−0.5

0

0.5

1

1.5

2

Three Sample Paths

−5 −4 −3 −2 −1 0 1 2 3 4 5−0.4

−0.2

0

0.2

0.4

0.6

0.8

1

Covariance Kernel

−5 −4 −3 −2 −1 0 1 2 3 4 50

0.02

0.04

0.06

0.08

0.1

0.12

0.14

0.16

0.18

0.2

Spectral Measure

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Example III - Gaussian Covariance

f (x) =∑

n∈Nζn

xn√n!e−

x2

2

r(x) = e−x2

2

dρ(λ) =√πe−

λ2

2 dλ

0 1 2 3 4 5 6 7 8 9 10−3

−2

−1

0

1

2

3

Three Sample Paths

−2 −1.5 −1 −0.5 0 0.5 1 1.5 20

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

Covariance Kernel

−5 −4 −3 −2 −1 0 1 2 3 4 50

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

Spectral Measure

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Example IV - Exponential Covariance

r(x) = e−|x |

dρ(λ) = 2λ2+1

0 1 2 3 4 5 6 7 8 9 10−3

−2

−1

0

1

2

3

Three Sample Paths

−2 −1.5 −1 −0.5 0 0.5 1 1.5 20

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

Covariance Kernel

−5 −4 −3 −2 −1 0 1 2 3 4 50

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

2

Spectral Measure

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General Construction

ρ - a finite, symmetric, non-negative measure on T ∗

{ψn}n - ONB of L2ρ(T

∗)

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General Construction

ρ - a finite, symmetric, non-negative measure on T ∗

{ψn}n - ONB of L2ρ(T

∗)

ϕn(x) :=

T∗

e−ixλψn(λ)dρ(λ)

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DefinitionsExamplesGeneral Construction

General Construction

ρ - a finite, symmetric, non-negative measure on T ∗

{ψn}n - ONB of L2ρ(T

∗)

ϕn(x) :=

T∗

e−ixλψn(λ)dρ(λ)

f (t)d=∑

n

ζnϕn(t), where ζn are i.i.d. N (0, 1).

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DefinitionsExamplesGeneral Construction

General Construction

ρ - a finite, symmetric, non-negative measure on T ∗

{ψn}n - ONB of L2ρ(T

∗)

ϕn(x) :=

T∗

e−ixλψn(λ)dρ(λ)

f (t)d=∑

n

ζnϕn(t), where ζn are i.i.d. N (0, 1).

make sure that ϕn are R-valued.

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DefinitionPrehistoryHistoryMain Result

Persistence Probability

Definition

Let f be a GSP on T . The persistence probability of f up totime t ∈ T is

Pf (t) := P

(f (x) > 0, ∀x ∈ (0, t]

).

a.k.a. gap or hole probability (referring to gap between zeroes orsign-changes).

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DefinitionPrehistoryHistoryMain Result

Persistence Probability

Definition

Let f be a GSP on T . The persistence probability of f up totime t ∈ T is

Pf (t) := P

(f (x) > 0, ∀x ∈ (0, t]

).

a.k.a. gap or hole probability (referring to gap between zeroes orsign-changes).Question: What is the behavior of P(t) as t → ∞?

Guess: “typically” P(t) ≍ e−θt .

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Persistence Probability

Definition

Let f be a GSP on T . The persistence probability of f up totime t ∈ T is

Pf (t) := P

(f (x) > 0, ∀x ∈ (0, t]

).

a.k.a. gap or hole probability (referring to gap between zeroes orsign-changes).Question: What is the behavior of P(t) as t → ∞?

Guess: “typically” P(t) ≍ e−θt .

(Xn)n∈Z i.i.d. ⇒ PX (N) = 2−N

Yn = Xn+1 − Xn ⇒ PY (N) = 1(N+1)! ≍ e−N logN

Zn ≡ Z0 ⇒ PZ (N) = P(Z0 > 0) = 12

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Engineering and Applied Mathematics40’s - 60’s

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DefinitionPrehistoryHistoryMain Result

Engineering and Applied Mathematics40’s - 60’s

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Engineering and Applied Mathematics40’s - 60’s

1944 Rice - “Mathematical Analysis of Random Noise”.

Mean number of level-crossings (Rice formula)Behavior of P(t) for t ≪ 1 (short range).

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Engineering and Applied Mathematics40’s - 60’s

1944 Rice - “Mathematical Analysis of Random Noise”.

Mean number of level-crossings (Rice formula)Behavior of P(t) for t ≪ 1 (short range).

1962 Slepian - “One-sided barrier problem”.

Slepian’s Inequality:r1(x) ≥ r2(x) ≥ 0 ⇒ P1(t) ≥ P2(t).

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Engineering and Applied Mathematics40’s - 60’s

1944 Rice - “Mathematical Analysis of Random Noise”.

Mean number of level-crossings (Rice formula)Behavior of P(t) for t ≪ 1 (short range).

1962 Slepian - “One-sided barrier problem”.

Slepian’s Inequality:r1(x) ≥ r2(x) ≥ 0 ⇒ P1(t) ≥ P2(t).

1962 Longuet-Higgins

generalized short-range results to gaps between nearlyconsecutive zeroes.

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Engineering and Applied Mathematics40’s - 60’s

1962 Newell & Rosenblatt

If r(x) → 0 as x → ∞, then P(t) = o(t−α) for any α > 0.

If |r(x)| < ax−α then P(t) ≤

e−Ct if α > 1

e−Ct/ log t if α = 1

e−Ctα if 0 < α < 1

examples for P(t) > e−C√t log t ≫ e−Ct (r(x) ≍ x−1/2).

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Engineering and Applied Mathematics40’s - 60’s

1962 Newell & Rosenblatt

If r(x) → 0 as x → ∞, then P(t) = o(t−α) for any α > 0.

If |r(x)| < ax−α then P(t) ≤

e−Ct if α > 1

e−Ct/ log t if α = 1

e−Ctα if 0 < α < 1

examples for P(t) > e−C√t log t ≫ e−Ct (r(x) ≍ x−1/2).

There are parallel independent results in the Soviet industry andAcademia (e.g., by Piterbarg, Kolmogorov)

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DefinitionPrehistoryHistoryMain Result

Physics90’s - 00’s

New motivation from physics:

electrons in matter (point process simulated by zeroes)non-equilibrium systems (Ising, Potts, diffusion with randominitial conditions)

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Physics90’s - 00’s

New motivation from physics:

electrons in matter (point process simulated by zeroes)non-equilibrium systems (Ising, Potts, diffusion with randominitial conditions)

1998-2004 Bray, Ehrhardt, Majumdar (and others).

“independent interval approximation”“correlator expansion method”: a series expansion for thepersistence exponentnumerical simulations

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Probability and Analysis00’s-

2005-14 Hole probability for Gaussian analytic functions- in the plane (Sodin-Tsirelson 2005, Nishry 2010)- in the hyperbolic disc (Buckley, Nishry, Peled, Sodin - 2014)

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Probability and Analysis00’s-

2005-14 Hole probability for Gaussian analytic functions- in the plane (Sodin-Tsirelson 2005, Nishry 2010)- in the hyperbolic disc (Buckley, Nishry, Peled, Sodin - 2014)

2013 Dembo & Mukherjee:

no zeroes for random polynomials ↔ persistence of GSP

If r(x) ≥ 0, then exists limt→∞− log P(t)

t∈ [0,∞) (uses

Slepian).

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Probability and AnalysisBounds for the sinc kernel

Theorem (Antezana, Buckley, Marzo, Olsen 2012)

For the sinc-kernel process (r(t) = sinc(t)), there is a constantc > 0 such that

e−cN ≤ Pf (N) ≤ 1

2N,

for all large enough N.

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Probability and AnalysisBounds for the sinc kernel

Theorem (Antezana, Buckley, Marzo, Olsen 2012)

For the sinc-kernel process (r(t) = sinc(t)), there is a constantc > 0 such that

e−cN ≤ Pf (N) ≤ 1

2N,

for all large enough N.

Upper bound: notice (f (n))n∈Z are i.i.d., so

P(f > 0, on (0,N] ∩ R) ≤ P(f > 0, on (0,N] ∩ Z) =1

2N.

Lower bound: an explicit construction + computation.

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DefinitionPrehistoryHistoryMain Result

Main Result

Theorem (F. & Feldheim, 2013)

Let f be a GSP (on Z or R) with spectral measure ρ. Supposethat ∃a,m,M > 0 such that ρ has density in [−a, a], denoted byρ′(x), and

∀x ∈ (−a, a) : m ≤ ρ′(x) ≤ M.

Then ∃c1, c2 > 0 s.t. for all large enough N:

e−c1N ≤ Pf (N) ≤ e−c2N .

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Main Result

Theorem (F. & Feldheim, 2013)

Let f be a GSP (on Z or R) with spectral measure ρ. Supposethat ∃a,m,M > 0 such that ρ has density in [−a, a], denoted byρ′(x), and

∀x ∈ (−a, a) : m ≤ ρ′(x) ≤ M.

Then ∃c1, c2 > 0 s.t. for all large enough N:

e−c1N ≤ Pf (N) ≤ e−c2N .

Given in terms of ρ (not r).

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Main Result

Theorem (F. & Feldheim, 2013)

Let f be a GSP (on Z or R) with spectral measure ρ. Supposethat ∃a,m,M > 0 such that ρ has density in [−a, a], denoted byρ′(x), and

∀x ∈ (−a, a) : m ≤ ρ′(x) ≤ M.

Then ∃c1, c2 > 0 s.t. for all large enough N:

e−c1N ≤ Pf (N) ≤ e−c2N .

Given in terms of ρ (not r).

roughly,∫Tr(x)dx converges and is positive.

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DefinitionPrehistoryHistoryMain Result

Main Result

Theorem (F. & Feldheim, 2013)

Let f be a GSP (on Z or R) with spectral measure ρ. Supposethat ∃a,m,M > 0 such that ρ has density in [−a, a], denoted byρ′(x), and

∀x ∈ (−a, a) : m ≤ ρ′(x) ≤ M.

Then ∃c1, c2 > 0 s.t. for all large enough N:

e−c1N ≤ Pf (N) ≤ e−c2N .

Given in terms of ρ (not r).

roughly,∫Tr(x)dx converges and is positive.

M is needed only for the upper bound.

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Main Result

Theorem (F. & Feldheim, 2013)

Let f be a GSP (on Z or R) with spectral measure ρ. Supposethat ∃a,m,M > 0 such that ρ has density in [−a, a], denoted byρ′(x), and

∀x ∈ (−a, a) : m ≤ ρ′(x) ≤ M.

Then ∃c1, c2 > 0 s.t. for all large enough N:

e−c1N ≤ Pf (N) ≤ e−c2N .

Given in terms of ρ (not r).

roughly,∫Tr(x)dx converges and is positive.

M is needed only for the upper bound.

Main tool: “spectral decomposition”

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Main Result

Theorem (F. & Feldheim, 2013)

Let f be a GSP (on Z or R) with spectral measure ρ. Supposethat ∃a,m,M > 0 such that ρ has density in [−a, a], denoted byρ′(x), and

∀x ∈ (−a, a) : m ≤ ρ′(x) ≤ M.

Then ∃c1, c2 > 0 s.t. for all large enough N:

e−c1N ≤ Pf (N) ≤ e−c2N .

(Xn)n∈Z i.i.d. ⇒ PX (N) = 2−N ρ′ = 1I[−π,π]

Yn = Xn+1 − Xn ⇒ PY (N) ≍ e−N logN ρ′ = 2(1 − cosλ)1I[−π,π]

Zn ≡ Z0 ⇒ PZ (N) =1

2ρ = δ0

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Spectral decompositionUpper boundLower bound

Ideas from the proof.

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Spectral decompositionUpper boundLower bound

Spectral decomposition

Key Observation

ρ = ρ1 + ρ2 ⇒ fd= f1 ⊕ f2,

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Spectral decompositionUpper boundLower bound

Spectral decomposition

Key Observation

ρ = ρ1 + ρ2 ⇒ fd= f1 ⊕ f2,

Proof:

cov((f1 + f2)(0), (f1 + f2)(x))

= cov(f1(0), f1(x)) + cov(f2(0), f2(x))

= ρ̂1(x) + ρ̂2(x) = ρ̂1 + ρ2(x) = cov(f (0), f (x)).

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Spectral decompositionUpper boundLower bound

Spectral decomposition

Key Observation

ρ = ρ1 + ρ2 ⇒ fd= f1 ⊕ f2,

Application:

ρ = m1I[−πk,π

k] + µ⇒ f = S ⊕ g

where rS (x) = c sinc( xk), and g is some GSP.

−10 −8 −6 −4 −2 0 2 4 6 8 100

0.5

1

1.5

2

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Spectral decompositionUpper boundLower bound

Spectral decomposition

Key Observation

ρ = ρ1 + ρ2 ⇒ fd= f1 ⊕ f2,

Application:

ρ = m1I[−πk,π

k] + µ⇒ f = S ⊕ g

where rS (x) = c sinc( xk), and g is some GSP.

−10 −8 −6 −4 −2 0 2 4 6 8 100

0.5

1

1.5

2

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Spectral decompositionUpper boundLower bound

Spectral decomposition

Key Observation

ρ = ρ1 + ρ2 ⇒ fd= f1 ⊕ f2,

Application:

ρ = m1I[−πk,π

k] + µ⇒ f = S ⊕ g

where rS (x) = c sinc( xk), and g is some GSP.

Observation.

(S(nk))n∈Z are i.i.d.

Proof: E[S(nk)S(mk)] = rS((m − n)k) = 0.

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Spectral decompositionUpper boundLower bound

Upper Bound

f = S ⊕ g , where (S(nk))n∈Z are i.i.d.

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Spectral decompositionUpper boundLower bound

Upper Bound

f = S ⊕ g , where (S(nk))n∈Z are i.i.d.

Let us use this observation to obtain an upper bound on Pf (N).

Pf (N) ≤ P

(S ⊕ g > 0 on (0,N]

∣∣∣ 1N

N∑

n=1

g(n) < 1

)

+ P

(1

N

N∑

n=1

g(n) ≥ 1

)

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Spectral decompositionUpper boundLower bound

Upper Bound

f = S ⊕ g , where (S(nk))n∈Z are i.i.d.

Let us use this observation to obtain an upper bound on Pf (N).

Pf (N) ≤ P

(S ⊕ g > 0 on (0,N]

∣∣∣ 1N

N∑

n=1

g(n) < 1

)

+ P

(1

N

N∑

n=1

g(n) ≥ 1

)

Lemma 1.

1N

∑Nn=1 g(n) ∼ NR(0, σ

2N), where σ

2N ≤ C0

N.

Here we use the upper bound M.

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Spectral decompositionUpper boundLower bound

Upper Bound

f = S ⊕ g , where (S(nk))n∈Z are i.i.d.

Let us use this observation to obtain an upper bound on Pf (N).

Pf (N) ≤ P

(S ⊕ g > 0 on (0,N]

∣∣∣ 1N

N∑

n=1

g(n) < 1

)

+ P

(1

N

N∑

n=1

g(n) ≥ 1

)

Lemma 1.

1N

∑Nn=1 g(n) ∼ NR(0, σ

2N), where σ

2N ≤ C0

N.

Here we use the upper bound M.

Lemma 1 ⇒ P( 1N

∑Nn=1 g(n) ≥ 1) ≤ e−c1N .

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Spectral decompositionUpper boundLower bound

Upper Bound

We may therefore assume 1N

∑Nn=1 g(n) < 1.

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Spectral decompositionUpper boundLower bound

Upper Bound

We may therefore assume 1N

∑Nn=1 g(n) < 1. Thus

for some ℓ ∈ {1, . . . , k}, we havek

N

⌊N/k⌋∑

n=0

g(ℓ+ nk) < 1.

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Spectral decompositionUpper boundLower bound

Upper Bound

We may therefore assume 1N

∑Nn=1 g(n) < 1. Thus

for some ℓ ∈ {1, . . . , k}, we havek

N

⌊N/k⌋∑

n=0

g(ℓ+ nk) < 1.

Lemma 2.

Let X1, . . . ,XN be i.i.d N (0, 1), and b1, . . . , bN ∈ R such that1N

∑Nj=1 bj < 1. Then ∃C > 0 so that

P (Xj + bj > 0, 1 ≤ j ≤ N) ≤ e−CN .

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Spectral decompositionUpper boundLower bound

Upper Bound

We may therefore assume 1N

∑Nn=1 g(n) < 1. Thus

for some ℓ ∈ {1, . . . , k}, we havek

N

⌊N/k⌋∑

n=0

g(ℓ+ nk) < 1.

Lemma 2.

Let X1, . . . ,XN be i.i.d N (0, 1), and b1, . . . , bN ∈ R such that1N

∑Nj=1 bj < 1. Then ∃C > 0 so that

P (Xj + bj > 0, 1 ≤ j ≤ N) ≤ e−CN .

Proof:logP(Xj ≥ −bj , 1 ≤ j ≤ N) = log

N∏

j=1

Φ(bj)

=

N∑

j=1

log Φ(bj) ≤ N log Φ

(1

N

∑bj

)≤ N log Φ(1).

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Spectral decompositionUpper boundLower bound

Lower bound

Reduction to functions: (f (j))j∈Z ❀ ρ ∈ M([−π, π]) ⊂ M(R),so may “extend” to (f (t))t∈R with the same ρ. Now,

P(f > 0 on (0,N] ∩ R) ≤ P(f > 0 on (0,N] ∩ Z).

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Spectral decompositionUpper boundLower bound

Lower bound

Reduction to functions: (f (j))j∈Z ❀ ρ ∈ M([−π, π]) ⊂ M(R),so may “extend” to (f (t))t∈R with the same ρ. Now,

P(f > 0 on (0,N] ∩ R) ≤ P(f > 0 on (0,N] ∩ Z).

First try: build an explicit event A ⊂ {f > 0 on (0,N]}.

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Spectral decompositionUpper boundLower bound

Lower bound

Reduction to functions: (f (j))j∈Z ❀ ρ ∈ M([−π, π]) ⊂ M(R),so may “extend” to (f (t))t∈R with the same ρ. Now,

P(f > 0 on (0,N] ∩ R) ≤ P(f > 0 on (0,N] ∩ Z).

First try: build an explicit event A ⊂ {f > 0 on (0,N]}.Second try: use known bounds. Recall:

f = S ⊕ g , where S is the (scaled) sinc-kernel process.

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Spectral decompositionUpper boundLower bound

Lower bound

Reduction to functions: (f (j))j∈Z ❀ ρ ∈ M([−π, π]) ⊂ M(R),so may “extend” to (f (t))t∈R with the same ρ. Now,

P(f > 0 on (0,N] ∩ R) ≤ P(f > 0 on (0,N] ∩ Z).

First try: build an explicit event A ⊂ {f > 0 on (0,N]}.Second try: use known bounds. Recall:

f = S ⊕ g , where S is the (scaled) sinc-kernel process.

P(S ⊕ g > 0 on (0,N])

≥ P(S > 1 on (0,N]) P(|g | ≤ 1

2on (0,N])

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Spectral decompositionUpper boundLower bound

Lower bound

Reduction to functions: (f (j))j∈Z ❀ ρ ∈ M([−π, π]) ⊂ M(R),so may “extend” to (f (t))t∈R with the same ρ. Now,

P(f > 0 on (0,N] ∩ R) ≤ P(f > 0 on (0,N] ∩ Z).

First try: build an explicit event A ⊂ {f > 0 on (0,N]}.Second try: use known bounds. Recall:

f = S ⊕ g , where S is the (scaled) sinc-kernel process.

P(S ⊕ g > 0 on (0,N])

≥ P(S > 1 on (0,N])︸ ︷︷ ︸ABMO

P(|g | ≤ 1

2on (0,N])

︸ ︷︷ ︸small ball prob.

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Spectral decompositionUpper boundLower bound

Lower bound

Lower bound on small ball probability:

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Spectral decompositionUpper boundLower bound

Lower bound

Lower bound on small ball probability:

Talagrand, Shao-Wang (1994), Ledoux (1996)

Suppose (X (t))t∈I is a centered Gaussian process on an interval I ,and

E|X (s)− X (t)|2 ≤ C |t − s|γ

for all s, t ∈ I and some 0 < γ ≤ 2, C > 0. Then

P(supt∈I

|X (t)| ≤ ε) ≥ exp

(−K |I |ε2/γ

)

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Spectral decompositionUpper boundLower bound

Lower bound

Lower bound on small ball probability:

Talagrand, Shao-Wang (1994), Ledoux (1996)

Suppose (X (t))t∈I is a centered Gaussian process on an interval I ,and

E|X (s)− X (t)|2 ≤ C |t − s|γ

for all s, t ∈ I and some 0 < γ ≤ 2, C > 0. Then

P(supt∈I

|X (t)| ≤ ε) ≥ exp

(−K |I |ε2/γ

)

For stationary processes, the moment condition is enough.

∃δ > 0 :

∫|λ|δdρ(δ) <∞.

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Spectral decompositionUpper boundLower bound

Further Research

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Spectral decompositionUpper boundLower bound

Further Research

spectral measure vanishes at 0

pointwise: P(N) ≍ e−cN logN?

on an interval: P(N) ≍ e−cN2

?

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Spectral decompositionUpper boundLower bound

Further Research

spectral measure vanishes at 0

pointwise: P(N) ≍ e−cN logN?

on an interval: P(N) ≍ e−cN2

?

spectral measure blows-up at 0: P(N) ≫ e−cN?

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Spectral decompositionUpper boundLower bound

Further Research

spectral measure vanishes at 0

pointwise: P(N) ≍ e−cN logN?

on an interval: P(N) ≍ e−cN2

?

spectral measure blows-up at 0: P(N) ≫ e−cN?

Prove existence of the limit

limN→∞

− logP(N)

N.

(recall known for r(t) ≥ 0: Dembo and Mukherjee).

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Spectral decompositionUpper boundLower bound

Further Research

spectral measure vanishes at 0

pointwise: P(N) ≍ e−cN logN?

on an interval: P(N) ≍ e−cN2

?

spectral measure blows-up at 0: P(N) ≫ e−cN?

Prove existence of the limit

limN→∞

− logP(N)

N.

(recall known for r(t) ≥ 0: Dembo and Mukherjee).

compute it.

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Spectral decompositionUpper boundLower bound

Thank you.“Persistence can grind an iron beam down into a needle.”

– – Chinese Proverb.