Heavy tailed and compactly supported distributions of quadratic Weyl sums with rational parameters Francesco CellarosiTariq Osman.

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Heavy tailed and compactly supported distributions
of quadratic Weyl sums with rational parameters
Francesco CellarosiTariq Osman.
January 27, 2023
Abstract
We consider quadratic Weyl sums SN(x;α, β) = PN
n=1 exp2πi 1
2n2+βnx+αn
for (α, β)Q2, where xRis randomly distributed according to a probability measure
absolutely continuous with respect to the Lebesgue measure. We prove that the limiting
distribution in the complex plane of 1
NSN(x;α, β) as N→ ∞ is either heavy tailed or
compactly supported, depending solely on α, β. In the heavy tailed case, the probability
(according to the limiting distribution) of landing outside a ball of radius Ris shown
to be asymptotic to T(α, β)R4, where the constant T(α, β)>0 is explicit. The result
follows from an analogous statement for products of generalized quadratic Weyl sums of
the form Sf
N(x;α, β) = PnZfn
Nexp2πi 1
2n2+βnx+αnwhere fis regular. The
precise tails of the limiting distribution of 1
NSf1
NSf2
N(x;α, β) as N→ ∞ can be described
in terms of a measure –which depends on (α, β)– of a super level set of a product of two
Jacobi theta functions on a noncompact homogenous space. Such measures are obtained
by means of an equidistribution theorem for rational horocycle lifts to a torus bundle over
the unit tangent bundle to a cover of the classical modular surface. The cardinality and
the geometry of orbits of rational points of the torus under the affine action of the theta
group play a crucial role in the computation of T(α, β). This work complements and
extends [6] and [32], in which the cases (α, β)/Q2and α=β= 0 are considered.
Contents
1 Introduction 2
2 Preliminaries 9
2.1 The Heisenberg Group and the Schr¨odinger Representation . . . . . . . . . . . . 9
2.2 f
SL(2,R) and the Shale-Weil Representation . . . . . . . . . . . . . . . . . . . . 9
2.3 From the Universal Jacobi Group to the Theta Function . . . . . . . . . . . . . 11
Department of Mathematics and Statistics. Queen’s University. Kingston, ON, Canada.
Corresponding author: fc19@queensu.ca
Department of Mathematics. Brandeis University. Waltham, MA, U.S.A.
1
arXiv:2210.09838v3 [math.NT] 25 Jan 2023
2.4 InvarianceProperties................................. 14
2.5 FundamentalDomains ................................ 15
2.6 Geodesic and Horocycle Flows . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15
2.7 Thekeyidentity.................................... 16
3 Invariant Measures 17
3.1 Five prototypical examples of orbits . . . . . . . . . . . . . . . . . . . . . . . . . 19
3.2 The Normalising Constants |S(α,β)|......................... 22
3.3 Symmetry....................................... 32
4 Limit Theorems 32
4.1 Rational Limit Theorems for Regular Indicators . . . . . . . . . . . . . . . . . . 32
4.2 Rational Limit Theorems for Sharp Indicators . . . . . . . . . . . . . . . . . . . 37
5 Growth in the Cusps and Tail Asymptotics 38
5.1 Tail asymptotics at i................................ 40
5.2 Tailasymptoticsat1................................. 43
5.3 Combined tail asymptotics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 47
6 The main constant 2|U(α,β)|+|V(α,β)|
|S(α,β)|47
6.1 The constant |U(α,β)|................................. 48
6.2 The constant |V(α,β)|................................. 49
6.3 The computation of the leading constant . . . . . . . . . . . . . . . . . . . . . . 51
7 The main theorems 53
7.1 The tails of the limiting distribution for regular indicators . . . . . . . . . . . . 53
7.2 The tails of the limiting distribution for sharp indicators . . . . . . . . . . . . . 54
8 Some numerical illustrations 58
References 61
1 Introduction
We consider quadratic Weyl sums of the form
SN(x;α, β) =
N
X
n=1
e1
2n2+βnx+αn,(1.1)
where e(z) = e2πiz,Nis a positive integer, and x,αand βare real. In our analysis, we fix α
and β, and we assume that xin (1.1) is randomly distributed on Raccording to a probability
measure λ, absolutely continuous with respect to the Lebesgue measure. We can understand
sums (1.1) as the position after Nsteps of a deterministic walk in Cwith a random seed x.
2
-4-2 0 2
-8
-6
-4
-2
0
α=1/5, β=1/3,
N=100, x=0.874663
-6-4-2 0 2 4 6
-8
-6
-4
-2
0
2
α=1/5, β=1/3,
N=100, x=0.317401
-2-101234
-6
-4
-2
0
α=1/5, β=1/3,
N=100, x=0.0418017
-8-6-4-2 0
-8
-6
-4
-2
0
α=1/5, β=1/3,
N=100, x=0.506402
-15 -10 -5 0
-2
0
2
4
6
8
α=1/2, β=3 ,
N=100, x=0.834469
0 2 4 6 8 10
0
2
4
6
8
10
α=1/2, β=3 ,
N=100, x=0.789321
-2-101234
-10
-5
0
α=1/2, β=3 ,
N=100, x=0.00687084
-20246
-2
0
2
4
6
8
α=1/2, β=3 ,
N=100, x=0.460187
-5-4-3-2-1 0 1
-6
-4
-2
0
2
4
α=1/6, β=1/6,
N=100, x=0.575034
-5 0 5 10 15
-10
-5
0
5
α=1/6, β=1/6,
N=100, x=0.332542
-15 -10 -5 0
-2
-1
0
1
2
3
4
α=1/6, β=1/6,
N=100, x=0.42748
-3-2-1 0 1 2 3 4
0
2
4
6
8
10
12
α=1/6, β=1/6,
N=100, x=0.0230083
-12 -10 -8-6-4-2 0
0
2
4
6
8
10
α=1/8, β=0,
N=100, x=0.032655
0 2 4 6 8
-2
0
2
4
α=1/8, β=0,
N=100, x=0.37372
-10 -8-6-4-2 0
-10
-5
0
α=1/8, β=0,
N=100, x=0.628386
-2 0 2 4 6
-2
0
2
4
α=1/8, β=0,
N=100, x=0.24871
Figure 1: Each panel represents the partial sums of (1.1), i.e. S1(x;α, β), S2(x;α, β), . . . , SN(x;α, β),
where N= 100 and α, β, x are specified in each panel. Each instance of xhas been randomly sampled
from the uniform measure on [0,1].
3
Each step is of length 1, and the n-th step is in the direction of e1
2n2+βnx+αn, see
Figure 1.
The emergence of spiral-like structures (curlicues) at various scales in the curves generated
by interpolating the partial sums (1.1) is well understood and can be explained by means
of an approximate functional equation. See, e.g., the works of Hardy–Littlewood [23] [22],
Mordell [37], Wilton [44], Fiedler–Jurkat–K¨orner [17], Deshouillers [10], Coutsias–Kazarinoff
[7] [8], Berry–Goldberg [1], Fedotov–Klopp [16], and Sinai [41]. We investigate the distribution
in the complex plane of the rescaled sums 1
NSN(x;α, β), as N→ ∞. Analyses along these
lines have been done already in several cases. Jurkat–van Horne [27] [28] [26] studied the
limiting distribution (in R) of 1
N|SN(x; 0,0)|when xis uniformly distributed on an interval
and found asymptotic formulas for all the moments (with explicit dependence on the interval)
as N→ ∞. The limiting distribution (in C) of 1
NSN(x; 0,0) was studied by Marklof [31]
[32] for general sampling measures λ. In [31], he also discussed the case β= 0 and found
that the limiting distribution depends on whether αis rational or irrational. The existence of
the limiting distributions (in Ck) of 1
NSbt1Nc(x; 0,0), Sbt2Nc(x; 0,0), . . . , SbtkNc(x; 0,0), where
0t1t2tk, was proven by Cellarosi [4]. An explicit limiting stochastic process for
t7→ 1
NSbtNc(x;α, β) was found by Cellarosi–Marklof [6] when (α, β)/Q2. In this case, it
was proven in [6] that the limiting distribution of 1
NSN(x;α, β) is heavy tailed. Specifically, if
(α, β)/Q2, we have
lim
N→∞ λnxR:1
N|SN(x;α, β)|> Ro=6
π2R61 + O(R12
31 )(1.2)
as R→ ∞. For comparison, when α=β= 0, it was shown in [32] that
lim
N→∞ λnxR:1
N|SN(x; 0,0)|> Ro=4 log 2
π2R4(1 + o(1)) (1.3)
as R→ ∞. Both (1.2)-(1.3) were recently sharpened by Cellarosi–Griffin–Osman [5] by replac-
ing the terms in parentheses by (1 + Oε(R2+ε)) for every ε > 0. For the limiting behaviour of
SN(x;α, β) for fixed xand random (α, β), see the work of Griffin–Marklof [20].
In this work we complement (1.2)-(1.3), as well as the results of [5], by considering arbitrary
(α, β)Q2. We focus on the leading behaviour of the tails of the limiting distribution and its
explicit dependence on (α, β). Before stating our results, let us introduce some notation.
Definition 1.0.1. Denote by {u} ∈ [0,1) the fractional part of a real number u. Given
(α, β)Q2, the numbers a, b, q Nsuch that {α}=a
q,{β}=b
q, and gcd(a, b, q) = 1 are
unique. We shall call qthe denominator of (α, β) and (a, b)∈ {0,1, . . . , q 1}2the numerators
of (α, β). Moreover, we shall refer to rationals pairs whose denominator is congruent to 2 modulo
4 and whose numerators are both odd as type C. In this case we shall write (α, β)C(2m) to
indicate that (α, β) has denominator 2mand is of type C(here mis necessarily odd). We shall
refer too all rational pairs that are not of type Cas type H. We shall write (α, β)H(q) to
indicate that the pair (α, β) has denominator qand is of type H.
4
Let us also introduce the Dedekind ψ-function
ψ(n) = nY
p|n1 + 1
p.(1.4)
We prove the following
Theorem 1.0.2. Let (α, β)Q2. Suppose λis a Borel probability measure on Rabsolutely
continuous with respect to Lebesgue measure. Let r1.
(i) If (α, β)C(2m), then there exists R0=R0(m, r)>0such that if R > R0then we have
lim
N→∞ λxR:1
NSNSbrN c(x;α, β)> R2= 0.(1.5)
In other words, the limiting distribution of 1
NSNSbrN c(·;α, β)is compactly supported.
(ii) If (α, β)H(q), then there exists T(q;r)>0such that
lim
N→∞ λxR:1
NSNSbrN c(x;α, β)> R2 T (q;r)R4,(1.6)
as R→ ∞. In particular, the limiting distribution of |1
NSNSbrN c(·;α, β)|has heavy tails.
Moreover, we have
T(q;r) = C(q)Drat(r)
π2,(1.7)
where, writing q= 2`mwith `0and modd,
C(q) =
2
ψ(m)if `= 0 or (`= 1 and either aor bis even);
1
2`1ψ(m)if ` > 1,
(1.8)
ψis as in (1.4), and
Drat(r) = (2 log 2 if r= 1;
2rcoth1(r) + 1
2log(r21) + r2
2log(1 1
r2)if r > 1.(1.9)
Example 1.0.3. The rational pairs (1
2,1
2),(1
6,1
6),(1
2,1
6) = (3
6,1
6),(5
6,1
2),(1
10 ,1
6) = ( 3
30 ,5
30 ) are all
of type C. Note that all integer pairs have denominator 1 and hence Z2=H(1). We have
C(1) = 2. A few more examples:
(0,1
2),(1
2,0),(3
2,0) H(2) and C(2) = 2,
(a
5,b
5)H(5) for all (a, b)Z2r(5Z)2and C(5) = 1
3,
(0,1
6),(1
3,1
6)=(2
6,1
6),(1
2,1
3)=(3
6,2
6)H(6) and C(6) = 1
2.
(3
2,4
5) = (15
10 ,8
10 )H(10) and C(10) = 1
3.
5
摘要:

HeavytailedandcompactlysupporteddistributionsofquadraticWeylsumswithrationalparametersFrancescoCellarosi*„TariqOsman….January27,2023AbstractWeconsiderquadraticWeylsumsSN(x; ; )=PNn=1exp2i12n2+ nx+ nfor( ; )2Q2,wherex2Risrandomlydistributedaccordingtoaprobabilitymeasureabsolutelycontinuouswithre...

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