DOI 10.1007/s00041-009-9115-8
Triangular Dirichlet Kernels and Growth of L
pLebesgue Constants
Marshall Ash
Received: 30 September 2009 / Published online: 24 December 2009
© Springer Science+Business Media, LLC 2009
Abstract LetP be a polygon inZ2and consider the mapping of anL1(T2)function into the partial sum of its Fourier series determined by the dilate ofP by the integer N. If the image space is endowed with theLp norm, 1< p <∞, then the operator norm will be given by theLpnorm of
(m,n)∈N Pe2π i(mx+ny). The size of this oper- ator norm is shown to beO(N2(1−1/p))when the polygon is a triangle. The estimate is independent of the shape of the triangle. For aksided polygon the corresponding estimate isO(kN2(1−1/p)).
Keywords Lebesgue constant·Dirichlet kernels in two dimensions·Dirichlet kernels for polygons
Mathematics Subject Classification (2000) Primary 42B15·42A05·Secondary 42A45
1 Introduction
In one dimension there is a very well known estimate [9]
1
0
N n=1
e2π nix dx 4
π2lnN. (1)
This integral is called the Lebesgue constant. In higher dimensions there are as many Lebesgue constants as there are generalizations of an interval of integers,
Communicated by Tom Körner.
M. Ash (
)DePaul University, Chicago, IL, USA e-mail:[email protected]
{1,2, . . . , N}. One such generalization is the set of two dimensional integer lattice points lying in the right triangle
Kθ,N=
x∈E2:x1+θ−1x2≤N, x1≥0, x2≥0 ,
whereEis the real numbers andθ∈(0,1]. In [8], A.A. Yudin and V.A. Yudin produce an estimate similar to relation (1) for this case. Reference [6] is also relevant here.
Whenp∈(1,∞), theL1relation (1) has a well knownLpanalogue, namely 1
0
N n=1
e2π nix
p
dx 2
π ∞
0
sinu u
pdu Np−1. (2) A sharp form of this appears as Lemma 1 of [1]. In Theorem1we extend what Yudin and Yudin did for the triangleKθ,N and theL1norm to the case of the same triangle Kθ,N and theLpnorm, for every finitep >1. The extension is routine except at one point where the easily verified inequality
d dx
N
n=1
e2π nix
≤CN
|x|, 0<|x| ≤1 2 proves to be useful.
An immediate corollary for an estimate of anL1or anLpLebesgue constant for a triangleKθ,N is a similar estimate for any two dimensional polygon. In theL1case, results for all polyhedrons in all dimensions are already known. See Chap. 6 of [5] for this. In Corollary2we state theLp result for polygons which follows immediately from Theorem1. Also results for all dimensions which include those found here when restricted to dimension two have been published recently [3]. However in contrast to the proof given here, the methods employed in [3] are not at all number theoretic.
Also the bounds established in [3], when specialized to two dimensions, are less precise than the bounds found here.
My original interest in this question came from studying a fundamental question from functional analysis: Is a commuting with translation operator of weak restricted type(2,2)necessarily bounded onL2(Z)? The affirmative answer to that question had a strong connection to this question: Given a subset of[0,1]of very small mea- sure, can one find a sum of exponentials with coefficients 0 or 1 whoseLp norm is largely concentrated on that subset? The result of this paper played an important role in the positive resolution of the second question. See [2] for explanations of these questions and their connections.
2 Results
Forn=(n1, n2)∈Z2, lete(nx)denote exp(2π i(n1x1+n2x2)).
Theorem 1 LetEbe the real numbers,θ∈(0,1]and Kθ,N =
x∈E2:x1+θ−1x2≤N, x1≥0, x2≥0 .
Then for each finitep >1 and arbitraryN≥1,
T2
n∈Kθ,N∩Z2
e (nx)
p
dx≤CpN2p−2
uniformly with respect toθandN.
Corollary 2 LetP be aksided polygon inE2of diameterN. Then
T2
n∈P∩Z2
e (nx)
p
dx≤kCpN2p−2.
The corollary is almost immediate since the polygon can be decomposed intok−2 triangles. See Theorem 2 in [8] for the details. So we pass immediately to the proof of the theorem.
Proof Upon settingM= N, we have
θ,N(x)=
n∈Kθ,N∩Z2
e (nx)= M n1=0
e (n1x1)
θ (N−n1) n2=0
e (n2x2)
since the upper edge of the triangle defining K is given by x1+θ−1x2=N, or x2=θ (N−x1). The inner sum is a geometric series sincee(n2x2)=e(x2)n2 so that we have
θ (N−n1) n2=0
e (n2x2)=e ((θ (N−n1) +1) x2)−1 e (x2)−1
and
θ,N(x)= M n1=0
e (n1x1)e ((θ (N−n1) +1) x2)−1 e (x2)−1 . Since
(θ (N−n1) +1)=θ (N−n1)+1− {θ (N−n1)}, where here, and hereafter,{· · · }will be reserved to mean fractional part;
θ,N(x)= M n1=0
e (n1x1)e ((θ (N−n1)+1) x2− {θ (N−n1)}x2)−1
e (x2)−1 .
But
e ((θ (N−n1)+1) x2− {θ (N−n1)}x2)−1
=e ((θ (N−n1)+1) x2)−1
+e ((θ (N−n1)+1) x2− {θ (N−n1)}x2)
−e ((θ (N−n1)+1) x2)
=e ((θ (N−n1)+1) x2)−1
=e ((θ (N−n1)+1) x2) (e (− {θ (N−n1)}x2)−1) , so
e (n1x1) (e ((θ (N−n1)+1) x2− {θ (N−n1)}x2)−1)
=e (n1x1) (e ((θ (N−n1)+1) x2)−1)
+e (n1(x1−θ x2)+(θ N+1)x2) (e (− {θ (N−n1)}x2)−1) , and
θ,N(x)= M n1=0
e (n1x1)e ((θ (N−n1)+1) x2)−1 e (x2)−1
+ M n1=0
e (n1(x1−θ x2)+(θ N+1)x2)e (− {θ (N−n1)}x2)−1 e (x2)−1
=J1(x)+J2(x) . We first estimate
I1=
T2|J1(x)|pdx.
For the Dirichlet kernelDn(x)=n
ν=0e(νx)=e(nx2)sin(π(nsinπ x+1)x), we use the esti- mates
D1 |Dn(x)| ≤n+1 n,
D2 |Dn(x)| ≤|2x1| |x|−1if 0<|x| ≤1/2, D3 |Dn(x)| ≤π n(n+1) n2,
D4 |Dn(x)| n|x|−1if 0<|x| ≤1/2.
Estimate D2 uses sinπ x ≥2x on [0,1/2]. Estimate D3 follows from |Dn| =
|n
ν=12π iνe(νx)| ≤2πn
ν=1ν. For D4, differentiate the closed form ofDn fac- tor oute(nx2)and then take|e(nx2)| =1 into account to get for 0<|x| ≤1/2,
Dn(x)=
π insinπ (n+1) x
sinπ x −πcosπ x
sin2π xsinπ (n+1) x + cosπ (n+1) x
sinπ x π (n+1)
≤ π n 1
2x +
π 1
(2x)2π (n+1) x +
1
2xπ (n+1) n
|x|.
Returning to the estimate ofI1, from
e (n1x1) (e ((θ (N−n1)+1) x2)−1)
=e ((θ N+1) x2) e (n1(x1−θ x2))−e (n1x1) and 1/|e (x2)−1| |x2|−1follows
I1
T2|x2|−p|e ((θ N+1) x2) DM(x1−θ x2)−DM(x1)|pdx. (3) Since
|e ((θ N+1) x2) DM(x1−θ x2)−DM(x1)|
= |e ((θ N+1) x2) DM(x1−θ x2)−DM(x1−θ x2) +DM(x1−θ x2)−DM(x1)|
≤ |e ((θ N+1) x2)−1| |DM(x1−θ x2)| + |DM(x1−θ x2)−DM(x1)|
= |2 sinπ (θ N+1) x2| · |DM(x1−θ x2)| + |DM(x1−θ x2)−DM(x1)|. (4) So to boundI1, it suffices to boundIAandIB, where
IA=
T2|x2|−p 2 sin1
2(θ N+1) x2
p|DM(x1−θ x2)|pdx, and IB=
T2|x2|−p|DM(x1−θ x2)−DM(x1)|pdx.
First, the change of variablex1=x1−θ x2,x2=x2has Jacobian 1, so IA=
T|DM(x1)|pdx1
T|x2|−p|2 sinπ (θ N+1) x2|pdx2.
The first integral is O(Np−1) by Lemma 2 of [1], and the substitution u = π(θ N+1)x2shows that the second integral is
∞
0
− ∞
π (θ N+1)
u π (θ N+1)
−p|2 sinu|p du π (θ N+1)
=cp(θ N+1)p−1−Ep,θ(N ) where cp =∞
0 (2πsinu u)p duπ and |Ep,θ(N )| (θ N +1)p−1∞
π(θ N+1)u−pdu=
π−p+1
p−1 . So uniformly inθ,
IA=Op
N2p−2
.
We now turn to the problem of estimatingIB. For estimatingIBwe change nota- tion from(x1, x2)to(x, y)and fromdxtodxdy. We must estimate
IB= 1/2
−1/2
1/2
−1/2
|y|−p|DM(x−θy)−DM(x)|pdxdy.
We make two reductions. First it is enough to integrate over[0,1/2]2. This is because symmetry considerations show that 1/2
0
1/2
0 =0
−1/2
0
−1/2 and that the integrals over the other two quadrants are both equal to
1/2 0
1/2 0
|y|−p|DM(x+θy)−DM(x)|pdxdy.
The estimation of this last integral is very similar to, but slightly simpler than the other one, since the set where x andy are big but x−θy is small needs special consideration in the first case, while the set wherexandyare big butx+θyis small is empty in the second case. Thus we only need to estimate
1/2 0
1/2 0
|y|−p|DM(x−θy)−DM(x)|pdxdy.
We may also assume thatθ=1, for making the substitutionx=x, y=θygives θp−1
θ/2 0
θ/2 0
|y|−p|DM(x−y)−DM(x)|pdxdy,
which is certainly dominated by 1/2
0
1/2
0
|y|−p|DM(x−y)−DM(x)|pdxdy,
uniformly forθ∈(0,1].
Partition[0,1/2]2into five parts,R, S, T , U, V. A picture is useful:U= [0,N2] × [0,N1] is the lower left corner,V is the remainder of the bottom strip of thickness N−1,S is the remainder of the left strip of thicknessN−1. The remaining square with lower left corner(N−1, N−1)and upper right corner(1/2,1/2)is made up of T, a thin diagonal strip whose upper boundary lies on the line y−x =N−1 and whose lower boundary lies on the liney−x= −N−1and ofR, a union of an upper left triangle and a lower right triangle.
First, sinceSis whereN−1< yand 0< x < N−1, then
S
1/2
N−1
1 yp
N−1 0
(N+N )pdx
dy
y−p+1|N1/2−1
NpN−1=O
N2p−2
.
Second,Ris where all ofx, y,and|x−y|are> N−1so that
R
1/2
N−1
1 yp
1/2 N−1
1
|x−y|+1 x
p
dx
dy 1/2
N−1
1 yp
1/2 N−1
1 tpdt
dy+
1/2 N−1
1 yp
1/2 N−1
1 xpdx
dy
=2
y−p+1|N1/2−1 x−p+1|N1/2−1
=O
N2p−2
.
Notice that here and elsewhere we usef +gpp≤2p(fpp+ gpp), which we sometimes write in the formf+gpp fpp+ gpp.
Third,T is where|x−y|< N−1, butx > N−1andy > N−1so that
T
T
1
yp N+1
x
p
dx dy 1/2
N−1
1 yp
Ly
Npdt
dy+ 1/2
N−1
1 yp
Ly
1 xpdx
dy
=2
y−p+1|N1/2−1 Np−1+Np−1 =O
N2p−2
,
where for the first integral we use|Ly| = |{(x, y)∈T}| =O(N−1)and for the second one we use inf{x:(x, y)∈Ly}> N−1.
Next,Uis wherex <2N−1, y∈(0, N−1), so the estimate
|DM(x−y)−DM(x)| ≤supDM |y| yields
U
N−1
0
1 yp
2N−1 0
N2y
p
dx
dy
=O
N2pN−1N−1 =O
N2p−2
.
What remains isV, wherex >2N−1, y < N−1and we must estimate
V
= N−1
0
1/2 2N−1
1
yp|DM(x−y)−DM(x)|pdx
dy.
Apply the mean value inequality|DM(x−y)−DM(x)| ≤sup|DM||y|and estimate (D4) to get
V = N−1
0
1/2 2N−1
1
yp|DM(x−y)−DM(x)|pdx
dy N−1
0
1/2 2N−1
1 yp
Mpyp inf0<t <y|x−t|pdx
dy
Mp N−1
0
dy ∞
2N−1
1
xpdx NpN−1Np−1=N2p−2, sincex >2N−1andy < N−1implies that
0<t <yinf |x−t| =x−y≥x 2x.
This completes the proof thatIBisO(N2p−2). So we conclude that I1=Op
N2p−2
. (5)
It remains to show that I2=
T2|J2(x)|pdx=O
N2p−2
.
Since
|J2(x)| = |e ((θ N+1)x2)|
M n1=0
e (n1(x1−θ x2))e (− {θ (N−n1)}x2)−1 e (x2)−1
=
M n1=0
e (n1(x1−θ x2))e (− {θ (N−n1)}x2)−1 e (x2)−1
, I2
T2
1
|x2|p
M n1=0
e (n (x1−θ x2)) (e (− {θ (N−n)}x2)−1)
p
dx
≤
T2
1
|x2|p
M n=0
e (n (x1−θ x2)) ∞ s=1
(−2π ix2)s({θ (N−n)})s s!
p
dx
≤
T2
∞
s=1
(2π )s s!
M n=0
e (n (x1−θ x2)) ({θ (N−n)})s
p
dx
=
T2
∞
s=1
(2π )s s!
M n=0
e (nx1) ({θ (N−n)})s
p
dx.
Denoting(
T2|f|p)1/pbyfpthe last inequality is I21/p
∞ s=1
(2π )s s!
M n=0
e (nx1) ({θ (N−n)})s p
so by Minkowski’s inequality, I21/p
∞ s=1
(2π )s s!
M n=0
e (nx1) ({θ (N−n)})s
p
which can be rewritten as I21/p
∞ s=1
(2π )s s!
⎛
⎝
T2
M n=0
e (nx1) ({θ (N−n)})s
p
dx
⎞
⎠
1/p
=∞
s=1
(2π )s s!
⎛
⎝
T
M n=0
e (nx) ({θ (N−n)})s
p
dx
⎞
⎠
1/p
= ∞ s=1
(2π )s s!
Hp,θ,N(s)1/p
.
In the penultimate step, we used
T2|f (x1)|dx1dx2=1 0dx2
1
0|f (x1)|dx1=1· 1
0|f (x)|dx. We now have to find a good estimate forHp,θ,N(s).
If we knew that
Hθ,N(s) Np−1lnps+Np−1lnpN+ sp N3p, then we would have
I21/p ∞ s=1
(2π )s s!
N1−1/plns+N1−1/plnN+ s N3
= ∞
s=1
(2π )slns s!
N1−1/p+ ∞
s=1
(2π )s s!
N1−1/plnN
+ ∞
s=1
(2π )s (s−1)!
N−3
=Op
N1−1/plnN
, (6)
I2 Op
Np−1lnpN
(7) since the infinite sums are constants for eachp. Finally estimates (5) and (7) prove
the theorem.
Lemma 3
Hp,θ,N(s) Np−1lnps+Np−1lnpN+ sp N3p. Proof Let us set=M−4and
ϕ(u)=
us 0≤u≤1−,
1
(1−)s(1−u) 1−≤u≤1, and extend it to be 1-periodic. Expandϕinto its Fourier series:
ϕ(u)= ˆ
ϕ(ν) e (νx) .
The Fourier coefficients satisfy
(1) | ˆϕ(ν)| ≤1, ν∈Z,
(2) | ˆϕ(ν)| ≤ |ν|−1Varϕ |ν|−1, ν=0, (3) | ˆϕ(ν)| ≤ |ν|−2Varϕ s−1|ν|−2, ν=0.
To see (1), notice thatϕ is nonnegative and continuous and has its maximum value on[0,1]atx=1− and that value is(1−)s which is bounded by 1. To see (2), notice thatϕ is monotone increasing on[0,1−]and monotone (linearly) decreasing on[1−,1]so its total variation is bounded by (2). To see (3), notice that
ϕ(u)=
sus−1 0< u <1−,
−1(1−)s 1− < u <1,
so the total variation ofϕ is the rise ofs(1−)s−1from 0+to(1−)− plus the jump ofs(1−)s−1−(−1(1−)s)atx=1−plus the jump of1(1−)satx=1.
All three of these quantities are s−1.
Further setA= {n∈Z∩ [0, M] : {θ (N−n)} ≤1−}and letA¯=Z∩ [0, M] \A be the complement ofAin{0,1,2, . . . , M}. Then
Hp,θ,N(s)=
T
M n=0
e (nx) ({θ (N−n)})s
p
dx
T
n∈A
e (nx) ({θ (N−n)})s
p
dx
+
T
n∈ ¯A
e (nx) ({θ (N−n)})s
p
dx
=G1+G2.
Sinceϕ(θ (N−n))= {(θ (N−n))}s for{(θ (N−n))} ≤1−,we have
G1=
T
n∈A
ϕ(θ (N−n)) e (nx)
p
dx,
G1/p1 =
n∈A
ϕ(θ (N−n)) e (nx) p
=
n∈A
ν∈Z
ˆ
ϕ(ν) e (νθ (N−n)) e (nx) p
≤
ν∈Z
ϕˆ(ν)
e (νθ N )
n∈A
e (n (x−νθ )) p
.
But observing|e(νθ N )| =1, making the variable changex=x−νθ, notingA¯= {0,1, . . . , M} \A, and applying Minkowski’s inequality gives
e (νθ N )
n∈A
e (n (x−νθ )) p
=
n∈A
e (n (x−νθ )) p
=
n∈A
e (nx) p
=
M n=0
e (nx)−
n∈ ¯A
e (nx) p
≤
M n=0
e (nx) p
+
n∈ ¯A
e (nx) p
,
so
G1≤2p
ν∈Z
ϕˆ(ν)p
T
M n=0
e (nx)
p
dx+
T
n∈ ¯A
e (nx) pdx
.
We use the estimates
|DM|p=O(Np−1t )and ∞
ν=−∞
ϕˆ(ν)=ϕˆ(0)+
1≤|ν|≤s
+
|ν|>s
1+
1≤|ν|≤s
1
|ν|+
|ν|>s
1
|ν|2
1+ln s
+1/
s
=1+ln(sM4)+ 1 sM4 ln(sN ) ,
and our estimate forG1becomes G1 ln(sN )
⎛
⎝Np−1+
T
n∈ ¯A
e (nx)
p
dx
⎞
⎠. (8) Turning toG2, forn∈ ¯A,{(θ (N−n))}>1−, so that
{(θ (N−n))}s> (1−)s and
1− {(θ (N−n))}s=1− {(θ (N−n))}s
<1−(1−)s
≤s.
Therefore
G2=
T
n∈ ¯A
e (nx)
1+ {θ (N−n)}s−1
p
dx
=
T
n∈ ¯A
e (nx)+
n∈ ¯A
e (nx)
{θ (N−n)}s−1
p
dx
≤2p
⎛
⎝
T
n∈ ¯A
e (nx)
p
dx+((M+1) s)p
⎞
⎠.
But=M−4so
G2
T
n∈ ¯A
e (nx)
dx+ sp
N3p. (9)
Our final assertion is that
T
n∈ ¯A
e (nx)
p
dx Np−1. (10)
If (10) holds, then from (8)
Hp,θ,N(s)≤ G1+G2 lnp(sN )
Np−1+Np−1 + sp
N3p+Np−1 Np−1lnps+Np−1lnpN+ sp
N3p,
since lnpsN=(lns+lnN )p lnps+lnpN, which finishes the lemma and hence the theorem. So all that remains is the verification of relation (10).
The idea of the rest of the proof is to show that the elements ofA¯lie in an arith- metic progression (or possibly in 2 of them), from which (10) is obvious. Explicitly, ifA¯= {a+b,2a+b, . . . , ka+b} ∪ {c+d,2c+d, . . . , kc+d}, then
T
n∈ ¯A
e (nx)
p
dx≤2p
T
k j=1
e ((j a+b) x)
p
dx
+2p
T
j=1
e ((j c+d) x)
p
dx
=2p 1
0
k j=1
e ((j a) x)
p
dx+2p 1
0
j=1
e ((j c) x)
p
dx
=2p1 a
a
0
k j=1
e (jy)
p
dy+2p1 c
c
0
j=1
e (jy)
p
dy
=2p 1
0
k j=1
e (jy)
p
dy+2p 1
0
j=1
e (jy)
p
dy
=Op(Np−1).
Thus it only remains to prove the following lemma.
Lemma 4 Let N be a positive real number and letθ∈(0,1]. Let M= Nand =M−4. ThenA¯= {n∈ {0,1, . . . , M} :1− <{θ (N−n)}<1}is an arithmetic progression or the union of two arithmetic progressions.
Proof We distinguish two cases,θirrational andθrational.
Case 1.θirrational.
Let{Qk:k=1,2, . . .}be the sequence of denominators of the convergents of the continued fraction expansion ofθ. Define the positive integerk0by
Qk0≤M < Qk0+1.
Letn1, n2∈ ¯A. Then from{θ (N−n1)}>1−and{θ (N−n2)}>1−we get θ (n1−n2) =min
∈Z|θ (n1−n2)−|
≤ |(θ (N−n2)−θ (N−n1))−(k2−k1)|
= |{θ (N−n2)} − {θ (N−n1)}|
where{θ (N−ni)} =θ (N−ni)−ki for integerski. Thus θ (n1−n2)< = 1
M4, (11)
where · denotes the distance to the nearest integer.
Since|n1−n2| ≤M, there is anm,1≤m≤Msuch that
θ m< . (12)
From elementary number theory we will need the following three facts.
LetPk/QkandPk+1/Qk+1be successive convergents ofθ. Then
Ifm < Qk+1, then for all∈Z, |θ m−| ≥ |θ Qk−Pk|, (13)
|θ Qk−Pk|> 1 Qk+Qk+1
, (14)
θ− Pk Qk
< 1 QkQk+1
. (15)
See Theorem 7.13 of [7] for the first fact, Theorem 13 in Khinchin’s book [4] for the second, and Theorem 7.11 of [7] for the third.
Next we estimateθ mfrom below. Sincem≤M < Qk+1, from facts (13) and (14) we get
θ m =min
∈Z|θ m−|> 1
Qk0+Qk0+1. (16) Putting (16) together with (12), gives
1
M4 = > 1
Qk0+Qk0+1≥ 1 M+Qk0+1
.
This is only possible ifQk0+1isO(M4); explicitly, from this we get M+Qk0+1> M4,
Qk0+1> M4−M, so that as soon asM≥2,
Qk0+1≥1
2M4. (17)
We show that ifn1, n2∈ ¯A, then n1−n2≡0 (mod Qk0). Indeed let n2−n1= qQk0+r, where 0< r < Qk0. Then
θ (n1−n2) =θ
qQk0+r
≥ θ r −θ qQk0
≥ θ r −qθ Qk0. (18) For the last step, note that for any norm and any integerq,
qa = a+ · · · +a
≤ a + · · · + a =qa. We also have
θ r ≥ 1
2Qk0; (19)
since applying facts (13) and (14) withk=k0−1 gives θ r =min
∈Z|θ r−|
> 1 Qk0−1+Qk0
> 1 Qk0+Qk0.
Also
θ Qk0= Qk0
Pk0 Qk0 +
θ Qk0−Qk0
Pk0 Qk0
= Pk0+
θ− Pk0
Qk0 Qk0
=
θ− Pk0 Qk0 Qk0
≤Qk0
θ− Pk0
Qk0
≤Qk0
θ− Pk0
Qk0
< Qk0
1
Qk0Qk0+1 = 1 Qk0+1. Taking this and inequality (19) into account,
θ r −qθ Qk0≥ 1
2Qk0 −q 1 Qk0+1
.
Combining this with (18) we have
θ (n1−n2) ≥ 1 2Qk0
−q 1 Qk0+1
.
TakingQk0≤M,q≤Mand (17) into account, from this we get θ (n1−n2) ≥ 1
2M−M 1
1/2M4
= 1/2M3−2M
M4 .
As soon asM≥3, this is contrary to
θ (n1−n2)< = 1 M4.
Consequently all theni are congruent modQk0 and there is a singler, 0≤r < Qk0 so that to everyn∈ ¯Athere corresponds aq so that
n=qQk0+r.
Let us consider the sequencexq,0≤q≤t= MQ−kr
0 , where for each integerq,xq= {θ (N−(qQk0+r))}is on the circle of circumference 1. Ifq1=q2, thenθirrational implies thatθ (N−(q2Qk0+r))−θ (N−(q1Qk0+r))=θ (q1−q2)Qk0 is not an integer, so thatxq1=xq2.