Quantitative Oppenheim theorem. Eigenvalue spacing for rectangular billiards. Pair correlation for higher degree diagonal forms

Similar documents
The Berry-Tabor conjecture

Applications of measure rigidity: from number theory to statistical mechanics

Applications of homogeneous dynamics: from number theory to statistical mechanics

Quantum Billiards. Martin Sieber (Bristol) Postgraduate Research Conference: Mathematical Billiard and their Applications

Eigenvalue statistics and lattice points

Analytic Number Theory

Roth s Theorem on Arithmetic Progressions

A genus 2 characterisation of translation surfaces with the lattice property

Quantum ergodicity. Nalini Anantharaman. 22 août Université de Strasbourg

Eigenvalues and eigenfunctions of the Laplacian. Andrew Hassell

Hilbert Spaces. Contents

Decouplings and applications

Kernel Method: Data Analysis with Positive Definite Kernels

Character sums with Beatty sequences on Burgess-type intervals

DECOUPLING INEQUALITIES IN HARMONIC ANALYSIS AND APPLICATIONS

ASYMPTOTIC DIOPHANTINE APPROXIMATION: THE MULTIPLICATIVE CASE

PAIR CORRELATION FOR QUADRATIC POLYNOMIALS MOD 1

THE SUM OF DIGITS OF PRIMES

MATH 205C: STATIONARY PHASE LEMMA

Large Sieves and Exponential Sums. Liangyi Zhao Thesis Director: Henryk Iwaniec

The Sommerfeld Polynomial Method: Harmonic Oscillator Example

NORMAL NUMBERS AND UNIFORM DISTRIBUTION (WEEKS 1-3) OPEN PROBLEMS IN NUMBER THEORY SPRING 2018, TEL AVIV UNIVERSITY

Properties of an infinite dimensional EDS system : the Muller s ratchet

Quadratic forms of signature (2, 2) and eigenvalue spacings on rectangular 2-tori

Chaos, Quantum Mechanics and Number Theory

Finite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product

Abstract. 2. We construct several transcendental numbers.

Topics in Fourier analysis - Lecture 2.

Estimates for the resolvent and spectral gaps for non self-adjoint operators. University Bordeaux

A gentle introduction to Quantum Ergodicity

Alexander Ostrowski

Harmonic sets and the harmonic prime number theorem

The two-point correlation function of the fractional parts of n is Poisson

Chapter 1. Preliminaries. The purpose of this chapter is to provide some basic background information. Linear Space. Hilbert Space.

Fractal uncertainty principle and quantum chaos

1 Definition of the Riemann integral

Continued Fraction Digit Averages and Maclaurin s Inequalities

1 The functional equation for ζ

1. Stochastic Processes and filtrations

Arithmetic quantum chaos and random wave conjecture. 9th Mathematical Physics Meeting. Goran Djankovi

Equations with regular-singular points (Sect. 5.5).

Dept of Math., SCU+USTC

The Gaussian free field, Gibbs measures and NLS on planar domains

Your first day at work MATH 806 (Fall 2015)

Using Spectral Analysis in the Study of Sarnak s Conjecture

Small Ball Probability, Arithmetic Structure and Random Matrices

Random Matrix: From Wigner to Quantum Chaos

EQUIDISTRIBUTION OF POLYNOMIAL SEQUENCES IN FUNCTION FIELDS, WITH APPLICATIONS. 1. Introduction

dynamical Diophantine approximation

MA5206 Homework 4. Group 4. April 26, ϕ 1 = 1, ϕ n (x) = 1 n 2 ϕ 1(n 2 x). = 1 and h n C 0. For any ξ ( 1 n, 2 n 2 ), n 3, h n (t) ξ t dt

On the distribution of lattice points on spheres and level surfaces of polynomials.

Ergodicity of quantum eigenfunctions in classically chaotic systems

Constructing Approximations to Functions

Quantum decay rates in chaotic scattering

Gaussian Random Fields

On the sup-norm problem for arithmetic hyperbolic 3-manifolds

Research Statement. Jayadev S. Athreya. November 7, 2005

Elements of Positive Definite Kernel and Reproducing Kernel Hilbert Space

Notes on Equidistribution

16 1 Basic Facts from Functional Analysis and Banach Lattices

Radial Basis Functions I

SCHWARTZ SPACES ASSOCIATED WITH SOME NON-DIFFERENTIAL CONVOLUTION OPERATORS ON HOMOGENEOUS GROUPS

The Simple Harmonic Oscillator

Random matrices and the Riemann zeros

Zero estimates for polynomials inspired by Hilbert s seventh problem

PATTERNS OF PRIMES IN ARITHMETIC PROGRESSIONS

H = ( H(x) m,n. Ω = T d T x = x + ω (d frequency shift) Ω = T 2 T x = (x 1 + x 2, x 2 + ω) (skewshift)

Recall that any inner product space V has an associated norm defined by

Computation of Rational Szegő-Lobatto Quadrature Formulas

An Invitation to Modern Number Theory. Steven J. Miller and Ramin Takloo-Bighash PRINCETON UNIVERSITY PRESS PRINCETON AND OXFORD

Lecture I: Asymptotics for large GUE random matrices

Atomic decompositions of square-integrable functions

1 Math 241A-B Homework Problem List for F2015 and W2016

Diophantine approximation of fractional parts of powers of real numbers

Asymptotic Behavior of the Magnetization Near Critical and Tricritical Points via Ginzburg-Landau Polynomials

A Note on Indefinite Ternary Quadratic Forms Representing All Odd Integers. Key Words: Quadratic Forms, indefinite ternary quadratic.

CENTRAL LIMIT THEOREM AND DIOPHANTINE APPROXIMATIONS. Sergey G. Bobkov. December 24, 2016

1.5 Approximate Identities

Topics in Harmonic Analysis Lecture 1: The Fourier transform

On the norm form inequality F (x) h.

Decoupling course outline Decoupling theory is a recent development in Fourier analysis with applications in partial differential equations and

Dirichlet s Theorem. Calvin Lin Zhiwei. August 18, 2007

Results of modern sieve methods in prime number theory and more

The Dirichlet problem for non-divergence parabolic equations with discontinuous in time coefficients in a wedge

Chapter 11. Taylor Series. Josef Leydold Mathematical Methods WS 2018/19 11 Taylor Series 1 / 27

Local semicircle law, Wegner estimate and level repulsion for Wigner random matrices

Skill 6 Exponential and Logarithmic Functions

From the mesoscopic to microscopic scale in random matrix theory

Analysis Comprehensive Exam Questions Fall 2008

Introduction to Ratner s Theorems on Unipotent Flows

Local Kesten McKay law for random regular graphs

Brownian Motion. 1 Definition Brownian Motion Wiener measure... 3

Linear Independence of Finite Gabor Systems

Cover Page. The handle holds various files of this Leiden University dissertation

Random and Deterministic perturbations of dynamical systems. Leonid Koralov

Chapter 29. Quantum Chaos

Manfred Einsiedler Thomas Ward. Ergodic Theory. with a view towards Number Theory. ^ Springer

Square Integrability of Gaussian Bells on Time Scales

Statistical signal processing

A survey on l 2 decoupling

Transcription:

QUANTITATIVE DISTRIBUTIONAL ASPECTS OF GENERIC DIAGONAL FORMS Quantitative Oppenheim theorem Eigenvalue spacing for rectangular billiards Pair correlation for higher degree diagonal forms

EFFECTIVE ESTIMATES ON INDEFINITE TERNARY FORMS Theorem (Dani Margulis) Let Q be an indefinite, irrational, ternary quadratic form. Then the set {Q(v) : v Z 3 primitive} is dense in the real line. There is the following quantification obtained by an effective version of Ratner s theorem. 2

Theorem (Lindenstrauss Margulis) Let Q be a given indefinite, ternary quadratic form with det Q = and ε > 0. Then, for T large enough, at least one of the following holds There is an integral quadratic form Q such that det Q < T ε and Q λq T where λ = det Q /3 For any ξ [ (log T ) c, (log T ) c], there is primitive v Z 3, 0 < v < T C such that Q(v) ξ (log T ) c 3

Let Q be as above. For which functions A(N) and δ(n) 0 (depending on Q) does the statement max min ξ <A(N) x Z 3 0< x <N Q(x) ξ < δ(n) hold? In the [L-M] result, A(N) and δ(n) depend logarithmically on N. Consider diagonal forms of signature (2, ) Q(x) = x 2 + α 2x 2 2 α 3x 2 3 (α 2, α 3 > 0) There is the stronger statement for one-parameter families ( ) Theorem (B) Let α 2 > 0 be fixed. For most α 3 > 0, the following holds (i) Assuming the Lindelöf hypothesis min x Z 3,0< x <N (ii) Unconditionally, Q(x) N +ε and ( ) holds provided A(N)δ(N) 2 N ε min x Z 3,0< x <N Q(x) N 2 5 +ε and ( ) holds assuming A(N) 3 δ(n) 2 N ε

REMARKS The statement min x Z 3,0< x <N Q(x) N +ε is essentially best possible For generic diagonal forms, i.e. considering both α 2 and α 3 as parameters, (i) holds without need of Lindelöf Ghosh and Kelmer obtained similar results for generic elements in the full space of indefinite ternary quadratic forms 5

EIGENVALUE SPACINGS OF FLAT TORI Berry Tabor Conjecture: local statistics of generic integrable quantum Hamiltonian coincide with those of random numbers generated by Poisson process PAIR CORRELATION FOR 2D FLAT TORI Γ R 2 lattice and M = R 2 /Γ associated flat torus. Eigenvalues of M given by 4π 2 v 2, v Γ (= dual lattice). These are the values at integral points of binary quadratic form B(m, n) = 4π 2 n v + n 2 v 2 2, with {v, v 2 } a Z-basis for Γ. Weyl law holds {j : λ j (M) T } c M T with c M = (area M )/4π Distribution of local spacings λ j λ k, j k R(a, b, T ) = { (j, k) : j k, λj T, λ k T, a λ j λ k b } T where < a < b <.

According to the Berry Tabor conjecture, λ j λ k (j k) should be uniformly distributed on R. Thus for given a < b, lim R(a, b, T ) = T c2 M (b a) ( ) Theorem (Sarnak, 996) space of all tori. ( ) holds for a set of full measure in the Analytical approach which seems to require 2 parameters and not applicable to rectangular billiards with eigenvalues αm 2 + n 2 (where α is the aspect ratio between height π and width π/ α). Theorem (Eskin-Margulis-Mozes) ( ) holds for (weakly) diophantine billiards, assuming 0 (a, b) In particular ( ) is valid for rectangular billiards provided α is diophantine, in the sense that qα > q C for some C > 0. Ergodic theory approach with no (or very poor) quantitative versions if we let b a 0 with T.

MINIMAL GAP FUNCTION OF SPECTRUM OF RECTANGULAR BILLIARD For α irrational, we get simple spectrum 0 < λ < λ 2 <, with growth {j : λ j T } = {(m, n); m, n, αm 2 + n 2 T } π 4 α T Definition δ (α) min (N) = min(λ i+ λ i : i N) For a Poisson sequence of N uncorrelated levels with unit mean spacing, the smallest gap is almost surely of size N. 8

Remark For the Gaussian unitary ensemble, on the scale of the mean spacing, smallest eigenphase gap is N /3, while for the Gaussian orthogonal ensemble, it is expected that the minimal gap is of size N /2. Theorem (Bloomer B Radziwill Rudnick) For almost all α > 0 δ (α) min (N) N ε δ (α) (log N)c min (N) N with c = log(e log 2) log 2 = 0, 086... infinitely often 9

PAIR CORRELATION FOR GENERIC 3D RECTANGULAR BILLIARDS Consider generic positive definite ternary quadratic form Q(x) = x 2 + αx2 2 + βx2 3 with α, β > 0. Restricting the variables to Z [0, N], mean spacing is O( N ). For T large and a < b, denote R(a, b; T ) = T 3/2 { (m, n) Z 3 + Z 3 + : m n, Q(m) T, Q(n) T and Q(m) Q(n) [a, b] } and c = lim ε 0 ε { (x, y) R 3 + R3 + ; Q(x) and Q(x) Q(y) < ε 2} 0

Theorem (B) Let Q = Q α,β with α, β > 0 parameters. Almost surely in α, β, the following holds. Fix 0 < ρ <. Let T and a < b, a, b < O() such that T ρ < b a <. Then R(a, b; T ) ct 2(b a) Remark Vanderkam established the pair correlation conjecture for generic four-dimensional flat tori using an unfolding procedure.

PAIR CORRELATION FOR HOMOGENOUS FORMS OF DEGREE k Let F (x,..., x k ) = x k + α 2x k 2 + + α kx k k with α 2,..., α k > 0. Thus average spacing between values of P is asymptotically constant. Define R(a, b; T ) = T { (m, n) Z k + Zk + : m n, F (m) T, F (n) T and F (m) F (n) [a, b]} Theorem (B) Consider α 2,..., α k as parameters. There is ρ > 0 such that almost surely in α 2,..., α k the following statement holds. Let T and a, b = O(), b a > T ρ. Then R(a, b; T ) c 2 (b a) where c = {x R k + : F (x) } Results of this type for generic elements in the full space of homogenous forms were obtained by Vanderkam (999) using Sarnak s method.

QUANTITATIVE OPPENHEIM FOR -PARAMETER FAMILIES Harmonic analysis approach but rather than expressing the problem using Gauss sums, reformulate it multiplicatively and rely on Dirichlet sum behavior. For instance, the sum n N is small for say t > N ε ; under the Lindelöf hypothesis one gets n N n it n it N 2( + t ) ε This permits to decompose in small and large t, where the small-t range provides main term and large-t contribution is an error term. 3

Consider one-parameter family Q α (x) = x 2 + x2 2 αx2 3 with α > 0 a parameter Taking x, x 2, x 3 N, condition x 2 + x2 2 αx2 3 < δ is rewritten as x 2 + x2 2 αx 2 3 δ N 2 or log(x 2 + x 2 2 ) 2 log x 3 log α The number of x, x 2, x 3 N for which this inequality holds is then expressed using Fourier transform as T t <T F (t) F 2 (2t) e it log α dt with T = N 2 δ δ N 2 F (t) = F 2 (t) = x,x 2 N x N x it (x 2 + x2 2 )it (partial sum of Epstein zeta function) (partial sum of Riemann zeta function)

Split t <T = t <N 2 + N 2< t <T = () + (2) Contribution of () amounts to δ N 2 N 2 x,x 2,x 3 N [ log(x 2 +x 2 2 ) 2 log x 3 log α <N 2] δn without further assumptions on α To bound contribution of (2), average in α and use Parseval T [ N 2< t <T ] F (t) 2 F 2 (t) 2 2 ( dt T 2 max N 2< t <T F 2 (t) ) (. T t <T ) F (t) 2 2 dt 5

Assuming Lindelöf For second factor T F (t) 2 dt t <T { max F 2(t) N 2T ε N ε < t <T # (x, x 2, x 3, x 4 ) Z 4 ; x i N and log(x 2 + x2 2 ) log(x2 3 + x2 4 ) < T # {(x, x 2, x 3, x 4 ) Z 4 ; x i N and x 2 + x2 2 x2 3 x2 4 < N 2 } T = δ N 2+ε This gives ( δ 2 cδn + O N.N ) 2 +ε N +ε δn provided N +ε < δ } 6

Unconditionally, one may show that a.s. in α min x Z 3 \{0} x <N Q α (x) N 2 5 +ε by bounding error term using distributional estimates. Main ingredients Large value estimate for Dirichlet polynomials Lemma Define S(t) = n M a n n it where a n. Then for T > M mes [ t < T : S(t) > V ] M ε (M 2 V 2 + M 4 V 6 T ) (due to Jutila, 977) Applied here with M = N 2 and S(t) = F 2 (t) 2. 7

Bounds on partial sums of the Epstein zeta function Lemma For t > N 2, one has the estimate m,n N (m 2 + n 2 ) it N t 3 +ε Follows the steps of Van der Corput s third derivative estimate, i.e. ( 6, 2 3 ) is a (2-dim) exponent pair Appears in a paper of V. Blomer on Epstein zeta functions where it is used to establish a bound E ( 2 + it ) t 3 +ε where E(s) = x Z 2 x 0 Q(x) s 8

SMALL GAPS IN SPECTRUM OF RECTANGULAR BILLIARD Recall that {λ < λ 2 < } = {αm 2 + n 2 : m, n Z} δ (α) min (N) = min (λ i+ λ i ) i N In order to bound δ (α) min (N), consider equivalently (M = N) min { n 2 n2 2 + α(n2 3 n2 4 ) : n i < M and (n, n 3 ) (n 2, n 4 ) } or min { n n 2 αn 3 n 4 : 0 < n i < M } ( ) Problem Is it true that ( ) M 2 ε for all α? In [B-B-R-R], this was shown for certain quadratic irrationals and also generically Proposition ( ) M 2 ε for almost all α.

Taking n i M, condition is replaced by SKETCH OF THE PROOF n n 2 αn 3 n 4 < δ log n + log n 2 log n 3 log n 4 log α < δ M 2 = T This leads to evaluation of T F t <T (t) 4 e it(log α) dt with F (t) = n it Split again t <T = t <M 2 + M 2< t <T n M = () + (2) Contribution of () evaluated independently of α and gives cδm 2 Contribution of (2) estimated in the α-mean and by Parseval bounded by 20

T [ Assuming Lindelöf, one obtains M 2< t <T F (t) 8 dt ] 2 M 2< t <T F (t) 8 dt T +ε M 4 leading to the condition δm 2 > T 2 +ε M 2, hence δ > M 2+ε. The Lindelöf hypothesis may be avoided in the following way. Replace n i M by n i = n i n i with n i M σ and n i M σ (σ arbitrary small and fixed). We obtain where T F (t) = t <T F (t) 4 G(t) 4 e it(log α) dt n M σ n it and G(t) = n it n M σ 2

Error term becomes Estimate T M 2< t <T F (t) 8 G(t) 8 dt M 2< t <T F (t) 8 G(t) 8 dt ( max M 2< t <T 2 G(t) 8 ). t <T F (t)4 2 dt This gives < M 8σ( τ) (T + M 4( σ) ) M 4( σ) for some τ = τ(σ) > 0 { (T δm 2 ε + O 2 + T M 2( σ) = δm 2 ε + O {(δ 2M } +2σ + δ)m 2 4στ ) M 2+2σ 4στ } and condition δ > M 2+4σ 22

The lower bound log(e log 2) Proposition For almost all α, letting c = log 2 = 0.086... δ (α) (log N)c min (N) N infinitively often uses K. Ford s result # { u.v : u, v Z +, u, v < N } 2 N(log N) c (log log N) 2/3 and shows small deviation from expected Poisson statistics for the eigenvalues. 23

PAIR CORRELATION FOR HOMOGENOUS DIAGONAL FORMS Recall that and R(a, b; T ) = T F (x,..., x k ) = x k + α 2x k 2 + + α kx k k (α i > 0) { (m, n) Z k + Zk + ; m n, F (m) T, F (n) T and F (m) F (n) [a, b]} A first step consists in a localization of the variables m i I i, n i J i where I i, J i are intervals of size T k 2ε satisfying a separation condition dist (I i, J i ) > T k ε. Let ξ = a+b 2 and δ = b a 2. Evaluate { (m, n) Z k Z k ; m i I i, n i J i and F (m) F (n) ξ < δ } ( ) T Condition F (m) F (n) ξ < δ is replaced by ( log m k n k +α 2(m k 2 nk 2 )+ +α k (m k k nk k ) ξ) log(m k k nk k ) log α δ k < α k = B where m k k nk k for m k I k, n k J k

Evaluate ( ) by S (t)s 2 (t) e it log α k ˆ [ B, B ] (t)dt ( ) with S (t) = ( m k n k + α 2(m k 2 nk 2 ) + + α k (m k k nk k ) ξ) it S 2 (t) = m i I i,n i J i m I k,n J k (m k n k ) it Set B 0 = α k T κ and decompose [ B, B ] = B 0 B [ B, 0 B ] + ( 0 [ B, B ] B 0 B ) [ B, 0 B ] producing in ( ) the main contribution and an 0 error term. Evaluation of the error term uses pointwise bound on S 2 (t) and an estimate T t <T S (t) 2 dt T 3 4 k +ε in average over α 2,..., α k 25

The following question seems open. Problem It is true that for all α R inf (m + n) mnα = 0? m,n Z + 26