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Badly approximable triangles and Delone sets

Shigeki Akiyama Institute of Mathematics, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki, 305-8571 Japan [email protected] Emily R. Korfanty Department of Mathematical and Statistical Sciences, University of Alberta, Edmonton, AB, T6G 2G1, Canada [email protected]  and  Yanli Xu Department of Mathematics and Statistics, Central China Normal University, Wuhan, 430079, China [email protected]
Abstract.

We investigate the linear equation x+y+z=1x+y+z=1 where πx\pi x, πy\pi y, πz\pi z are three angles of a triangle and the numbers xx, yy, zz are badly approximable. We show that there are exactly two solutions which have the smallest partial quotients by lexicographical ordering. Lastly, we give a construction of associated Delone sets which are expected to have rotationally invariant diffraction.

Key words and phrases: Badly approximable numbers, Hall’s ray, Iterated Function System, Delone sets, Chabauty–Fell topology.
* Corresponding author.

1. Introduction

Let x=mina|ax|\lVert x\rVert=\min_{a\in\mathbb{Z}}|a-x| denote the distance from a real number xx to the nearest integer. A real irrational number xx is called badly approximable if

infq+qqx>0.\inf_{q\in\mathbb{Z}_{+}}q\lVert qx\rVert>0.

It is a well known fact that an irrational number x(0,1)x\in(0,1) is badly approximable if and only if the partial quotients in the continued fraction expansion

x=[a1(x),a2(x),]=1a1(x)+1a2(x)+1,aj(x)+,j=1,2,,x=[a_{1}(x),a_{2}(x),\dots]=\cfrac{1}{a_{1}(x)+\cfrac{1}{a_{2}(x)+\cfrac{1}{\ddots}}}\,,\quad a_{j}(x)\in\mathbb{Z}_{+}\,,\ j=1,2,\ldots\,,

are bounded, i.e. if supk1ak(x)<\sup_{k\geq 1}a_{k}(x)<\infty. By using the Gauss map

T(x)=1x1x,T(x)=\frac{1}{x}-\left\lfloor\frac{1}{x}\right\rfloor\,,

we have

Tk1(x)=[ak(x),ak+1(x),ak+2(x),],T^{k-1}(x)=[a_{k}(x),a_{k+1}(x),a_{k+2}(x),\dots]\,,

and ak(x)=1/Tk1(x)a_{k}(x)=\lfloor 1/T^{k-1}(x)\rfloor for all k1k\geq 1.

In this work, we are interested in planar triangles where every angle is the product of π\pi and a badly approximable number. More specifically, our target is the equation

x+y+z=1,x+y+z=1\,,

where πx,πy,πz\pi x,\pi y,\pi z are the angles of the corresponding triangle and x,y,zx,y,z are badly approximable numbers. We are especially interested in solutions such that the partial quotients of xx, yy, zz are small by lexicographical ordering. In this case, we call πx,πy,πz\pi x,\pi y,\pi z optimal badly approximable angles.

Badly approximable angles often appear in phyllotaxis. One such example is the golden angle πω\pi\omega where

ω=512=[1,1,].\omega=\frac{\sqrt{5}-1}{2}=[1,1,\dots]\,.

When considering the irrational rotation tt+ψ(mod1)t\mapsto t+\psi\pmod{1}, the choice ψ=ω\psi=\omega achieves the minimum discrepancy of the sequence nψ(mod1)n\psi\pmod{1}, i.e. it gives the most uniform distribution in [0,1][0,1]. In general, if the maximum of the partial quotients of ψ\psi is small, then the discrepancy becomes small (c.f. [11, Chapter 2, Theorem 3.4]).

We first encountered this topic while exploring constructions of Delone sets with rotationally invariant diffraction patterns. Delone sets with this property can be derived from tilings with statistical circular symmetry involving angles that are incommensurable with π\pi. There are many tilings with statistical circular symmetry [8, 9, 15, 16]; however, in all of these examples, the angles are not known to be badly approximable. Motivated by this, we produce new Delone sets by triangles with optimal badly approximable angles. We essentially follow the threshold method for multiscale substitution schemes considered in [19], but we use contractions described by a graph directed iterated function system to give a concise presentation. The main idea is to subdivide the triangles until the areas reach a given threshold, and then renormalize them to obtain larger and larger patches. A different construction of Delone sets via badly approximable angles and Fermat Spirals is discussed in [1, 5, 13, 20].

We call the continued fraction

x=[a1,a2,],x=[a_{1},a_{2},\dots]\,,

periodic if there exist positive integers k0k_{0} and hh such that, for arbitrary kk0k\geq k_{0},

ak+h=ak.a_{k+h}=a_{k}\,.

In analogy with the common notation for periodic decimal expansions, we shall write such a periodic continued fraction as:

x=[a1,a2,,ak01,ak0,ak0+1,,ak0+h1¯].x=[a_{1},a_{2},\dots,a_{k_{0}-1},\overline{a_{k_{0}},a_{k_{0}+1},\dots,a_{k_{0}+h-1}}]\,.

We use the notation (ak0,ak0+1,,ak0+h1)(a_{k_{0}},a_{k_{0}+1},\dots,a_{k_{0}+h-1})^{\ell} to denote the repetition of the numbers ak0,ak0+1,ak0+h1a_{k_{0}},a_{k_{0}+1},\dots a_{k_{0}+h-1} in the continued fraction 0\ell\geq 0 many times. We write (aj)(a_{j})^{\ell} for the repetition of a single number aja_{j}. For convenience, in the case where x(0,1)x\in(0,1)\cap{\mathbb{Q}} we use the notation

x=[a1,a2,,an,]=1a1+1a2+1+1an.x=[a_{1},a_{2},\dots,a_{n},\infty]=\frac{1}{a_{1}+\frac{1}{a_{2}+\frac{1}{\ddots+\frac{1}{a_{n}}}}}\,.
Definition 1.1.

Define the cylinder set of b1,,bnb_{1},\dots,b_{n}\in\mathbb{N} by

I(b1,,bn)={x(0,1):x=[x1,x2,],xi=bifor 1in}.I(b_{1},\dots,b_{n})=\{x\in(0,1)\,:\,x=[x_{1},x_{2},\dots]\,,x_{i}=b_{i}\ for\ 1\leq i\leq n\}\,.

The set I(b1,,bn)I(b_{1},\dots,b_{n}) is an interval with endpoints

Pn+Pn1Qn+Qn1andPnQn,\frac{P_{n}+P_{n{\color[rgb]{0,0,1}-}1}}{Q_{n}+Q_{n{\color[rgb]{0,0,1}-}1}}\quad and\quad\frac{P_{n}}{Q_{n}}\,,

for n1n\geq 1, where

Pn=bnPn1+Pn2,Qn=bnQn1+Qn2,P_{n}=b_{n}P_{n-1}+P_{n-2}\,,\quad Q_{n}=b_{n}Q_{n-1}+Q_{n-2}\,,

with

(P1P0Q1Q0)=(1001).\begin{pmatrix}P_{-1}&P_{0}\\ Q_{-1}&Q_{0}\end{pmatrix}=\begin{pmatrix}1&0\\ 0&1\end{pmatrix}\,.

Let us define our linear problem for badly approximable numbers more precisely. An irrational number x(0,1)x\in(0,1) is BB-bad if ak(x)Ba_{k}(x)\leq B holds for all k1k\geq 1. Let B{\mathcal{B}}_{B} be the set of all BB-bad numbers in (0,1)\(0,1)\backslash{\mathbb{Q}}. For j0j\geq 0, we define the set

B,j=B+1Tj(B),{\mathcal{B}}_{B,j}={\mathcal{B}}_{B+1}\cap T^{-j}({\mathcal{B}}_{B})\,,

i.e., B,j{\mathcal{B}}_{B,j} is the set of irrational numbers which satisfy

{akB+1kjakBk>j.\begin{cases}a_{k}\leq B+1&k\leq j\\ a_{k}\leq B&k>j\,.\end{cases}

Clearly, we have

B=B,0B,1B,2.{\mathcal{B}}_{B}={\mathcal{B}}_{B,0}\subset{\mathcal{B}}_{B,1}\subset{\mathcal{B}}_{B,2}\subset\cdots\,.

Further, we define B=j=0B,j{\mathcal{B}}^{*}_{B}=\bigcup_{j=0}^{\infty}{\mathcal{B}}_{B,j} to be the set of eventually BB-bad numbers in B+1{\mathcal{B}}_{B+1}. In this paper, we are interested in the additive structure of B,j{\mathcal{B}}_{B,j} and B{\mathcal{B}}^{*}_{B}. We begin with a simple lemma.

Lemma 1.2.

For x=[a1,a2,a3,](0,1)x=[a_{1},a_{2},a_{3},\dots]\in(0,1), we have

1x={[1,a11,a2,a3,]a12[1+a2,a3,]a1=1.1-x=\begin{cases}[1,a_{1}-1,a_{2},a_{3},\dots]&a_{1}\geq 2\\ [1+a_{2},a_{3},\dots]&a_{1}=1\,.\end{cases}
Proof.

Putting x=1/(a1+y)x=1/(a_{1}+y) with y(0,1)y\in(0,1), we see that

1x=11+1a11+y,1-x=\cfrac{1}{1+\frac{1}{a_{1}-1+y}}\,,

from which the result easily follows.

Corollary 1.3.

An irrational number xx is in 2,1{\mathcal{B}}_{2,1} if and only if 1x1-x is also in 2,1{\mathcal{B}}_{2,1}.

Remark 1.4.

The property of 2,1{\mathcal{B}}_{2,1} described in Corollary 1.3 does not hold in 2{\mathcal{B}}_{2} or in 2,j{\mathcal{B}}_{2,j} for any j2j\geq 2.

Remark 1.5.

Lemma 1.2 shows that the equation x+y=1(x,y2,xy)x+y=1\ (x,y\in{\mathcal{B}}_{2},\ x\leq y) is trivially solved and has the set of solutions

{(x,1x)|x2[0,1/2)}.{\color[rgb]{0,0,1}\{(x,1-x)\ |\ x\in{\mathcal{B}}_{2}\cap[0,1/2)\}\,.}

In particular, the equation has uncountably many different solutions. However, our equation of interest x+y+z=1x+y+z=1 has no solutions in 2{\mathcal{B}}_{2}. Indeed, if x,y,z2x,y,z\in{\mathcal{B}}_{2}, then we also have x,y,zI(1)I(2)=[13,1)x,y,z\in I(1)\cup I(2)=[\frac{1}{3},1). However, if we also have x+y+z=1x+y+z=1, then the only possible solution is x=y=z=13x=y=z=\frac{1}{3}\in\mathbb{Q}, which contradicts irrationality of x,y,z2x,y,z\in{\mathcal{B}}_{2}.

Our main results are as follows:

Theorem 1.6.

The equality x+y+z=1(x,y,z2,1,xyz)x+y+z=1\ (x,y,z\in{\mathcal{B}}_{2,1},\ x\leq y\leq z) has exactly two solutions

x=23=[3,1,2¯],y=z=312=[2,1¯],x=2-\sqrt{3}=[3,\overline{1,2}],\ y=z=\frac{\sqrt{3}-1}{2}=[\overline{2,1}]\,,

and

x=y=222=[3,2¯],z=21=[2¯].x=y=\frac{2-\sqrt{2}}{2}=[3,\overline{2}],\ z=\sqrt{2}-1=[\overline{2}]\,.

By using Lemma 1.2, we may rephrase Theorem 1.6 as follows:

Theorem 1.7.

The equality x+y=z(x,y,z2,1,xy)x+y=z\ (x,y,z\in{\mathcal{B}}_{2,1}\,,x\leq y) has exactly four solutions

x=23=[3,1,2¯],y=312=[2,1¯],z=332=[1,1,1,2,1¯],x=2-\sqrt{3}=[3,\overline{1,2}],\ y=\frac{\sqrt{3}-1}{2}=[\overline{2,1}],\ z=\frac{3-\sqrt{3}}{2}=[1,1,1,\overline{2,1}]\,,
x=y=312=[2,1¯],z=31=[1,2¯],x=y=\frac{\sqrt{3}-1}{2}=[\overline{2,1}],\ z=\sqrt{3}-1=[\overline{1,2}]\,,
x=y=222=[3,2¯],z=22=[1,1,2¯],x=y=\frac{2-\sqrt{2}}{2}=[3,\overline{2}],\ z=2-\sqrt{2}=[1,1,\overline{2}]\,,

and

x=222=[3,2¯],y=21=[2¯],z=22=[1,2¯].x=\frac{2-\sqrt{2}}{2}=[3,\overline{2}],\ y=\sqrt{2}-1=[\overline{2}],\ z=\frac{\sqrt{2}}{2}=[1,\overline{2}]\,.

In 1954, Hall [10] proved that 4+4{\mathcal{B}}_{4}+{\mathcal{B}}_{4} contains an interval. Subsequently, Freiman [7] and Schecker [17] showed that 3+3{\mathcal{B}}_{3}+{\mathcal{B}}_{3} contains an interval. This implies that the equalities x+y+z=1(x,y,z3,xyz)x+y+z=1\ (x,y,z\in{\mathcal{B}}_{3},\ x\leq y\leq z) and x+y=z(x,y,z3,xy)x+y=z\ (x,y,z\in{\mathcal{B}}_{3},\ x\leq y) both have uncountably many solutions.

These results were proven using a criterion for Cantor sets which, when satisfied, implies that the arithmetic sum of two Cantor sets contains an interval. By this method, it may be challenging to make the solutions explicit, i.e. we know that one can choose any z3z\in{\mathcal{B}}_{3} in the interval, but it is not clear which numbers x,y3x,y\in{\mathcal{B}}_{3} satisfy the equation. In contrast, our method gives explicit solutions in 2{\mathcal{B}}^{*}_{2} and 3{\mathcal{B}}_{3}.

Theorem 1.8.

The equality x+y+z=1(x,y,z2,xyz)x+y+z=1\ (x,y,z\in{\mathcal{B}}^{*}_{2},\ x\leq y\leq z) has infinitely many solutions. Furthermore, uncountably many solutions of the equality x+y+z=1(x,y,z3,xyz)x+y+z=1\ (x,y,z\in{\mathcal{B}}_{3},\ x\leq y\leq z) can be constructed explicitly.

The paper is organized as follows. In Section 2, we prove Theorem 1.6 and 1.7. In Section 3, we prove Theorem 1.8. In Section 4, we return to the original motivation and discuss the construction of Delone sets using the optimal badly approximable angles found in Theorem 1.6. Finally, in Section 5, we give several open problems.

2. Proof of Theorems 1.6 and 1.7

To prove Theorem 1.6 and 1.7, we will need the following lemmas:

Lemma 2.1 (Forbidden patterns).

Let z(0,1)\z\in(0,1)\backslash{\mathbb{Q}} be such that z[r1,r2]z\in[r_{1},r_{2}] for some r1,r2(0,1)r_{1},r_{2}\in(0,1)\cap{\mathbb{Q}}. If the simple continued fractions of r1r_{1} and r2r_{2} are of the form

r1=[(2)2k1,(2,1),s,a1,,an1,],r2=[(2)2k1,b1,,bn2,],r_{1}=[(2)^{2k-1},(2,1)^{\ell},s,a_{1},\dots,a_{n_{1}},\infty]\,,\quad r_{2}=[(2)^{2k-1},b_{1},\dots,b_{n_{2}},\infty]\,, (2.1)

or

r1=[(2)2k,a1,,an1,],r2=[(2)2k,(2,1),s,b1,,bn2,],r_{1}=[(2)^{2k},a_{1},\dots,a_{n_{1}},\infty]\,,\quad r_{2}=[(2)^{2k},(2,1)^{\ell},s,b_{1},\dots,b_{n_{2}},\infty]\,, (2.2)

where k1k\geq 1, 0\ell\geq 0, and s3s\geq 3, then z2z\notin{\mathcal{B}}_{2}.

Proof.

Case 1. Assume that r1r_{1} and r2r_{2} are of the form (2.1) where k1k\geq 1, 0\ell\geq 0, and s3s\geq 3.

Let z=[c1,c2,]z=[c_{1},c_{2},\dots]. Suppose by contradiction that z2z\in{\mathcal{B}}_{2}. First, for simplicity, observe that (2.1) implies

[(2)2k1,(2,1),s,]z[(2)2k1,].[(2)^{2k-1},(2,1)^{\ell},s,\infty]\leq z\leq[(2)^{2k-1},\infty]\,. (2.3)

Since (2.1) requires c1,,c2k12c_{1},\dots,c_{2k-1}\geq 2 and z2z\in{\mathcal{B}}_{2} requires c1,,c2k12c_{1},\dots,c_{2k-1}\leq 2, we must have

c1==c2k1=2,c_{1}=\dots=c_{2k-1}=2\,, (2.4)

i.e. zI((2)2k1)z\in I((2)^{2k-1}).

Next, consider u=[c2k,c2k+1,]u=[c_{2k},c_{2k+1},\dots]. By (2.3) and (2.4), we have

u[(2,1),s,].u\leq[(2,1)^{\ell},s,\infty]\,. (2.5)

From this, we can deduce that uI((2,1))u\in I((2,1)^{\ell}). To see this, observe that (2.5) gives us c2k2c_{2k}\geq 2, so we must have c2k=2c_{2k}=2 because u2u\in{\mathcal{B}}_{2}. We also get that c2k+11c_{2k+1}\leq 1, so we must have c2k+1=1c_{2k+1}=1. Proceeding inductively, we find that c2q=2c_{2q}=2 and c2q+1=1c_{2q+1}=1 for kqk+1k\leq q\leq k+\ell-1.

Now consider v=[c2(k+),c2(k+)+1,]v=[c_{2(k+\ell)},c_{2(k+\ell)+1},\dots]. From (2.5) we get

v[s,]=1s,v\leq[s,\infty]=\frac{1}{s}\,,

so c2(k+)=1/vs3c_{2(k+\ell)}=\lfloor 1/v\rfloor\geq s\geq 3, contradicting v2v\in{\mathcal{B}}_{2}. Therefore, zz cannot have the form (2.1).

Case 2. The proof when r1r_{1} and r2r_{2} are of the form (2.2) is similar to Case 1. ∎

We call any interval of the form (2.1) or (2.2) a forbidden pattern. Moreover, if z[r1,r2]z\in[r_{1},r_{2}] for some forbidden pattern [r1,r2][r_{1},r_{2}], we say that zz is contained in a forbidden pattern.

Lemma 2.2.

The equality x+y=z(x,y,z2)x+y=z\ (x,y,z\in{\mathcal{B}}_{2}) has exactly one solution

x=y=312=[2,1¯],z=31=[1,2¯].x=y=\frac{\sqrt{3}-1}{2}=[\overline{2,1}],\ z=\sqrt{3}-1=[\overline{1,2}]\,. (2.6)
Proof.

Suppose x=[a1,a2,]x=[a_{1},a_{2},\cdots] where ai{1,2}a_{i}\in\{1,2\} with i1i\geq 1 and y=[b1,b2,]y=[b_{1},b_{2},\cdots] where bj{1,2}b_{j}\in\{1,2\} with j1j\geq 1. It is very easy to get that x<yx<y if and only if (1)nan<(1)nbn(-1)^{n}a_{n}<(-1)^{n}b_{n} for the first nn such that anbna_{n}\neq b_{n}. As a consequence, we have

312=[2,1¯]=min(2),\frac{\sqrt{3}-1}{2}=[\overline{2,1}]\,{\color[rgb]{0,0,1}=\min({\mathcal{B}}_{2})}\,,

and

31=[1,2¯]=max(2).\sqrt{3}-1=[\overline{1,2}]\,{\color[rgb]{0,0,1}=\max({\mathcal{B}}_{2})}\,.

With this preparation, we show that (2.6) is the unique solution of x+y=z(x,y,z2)x+y=z\ (x,y,z\in{\mathcal{B}}_{2}) by considering the sum of xx and yy.

If x+y<31x+y<\sqrt{3}-1, we get that one of them is less than 312\frac{\sqrt{3}-1}{2}, which contradicts 312\frac{\sqrt{3}-1}{2} being the minimum of 2{\mathcal{B}}_{2}. Thus, x+y31x+y\geq\sqrt{3}-1. Similarly, if x+y>31x+y>\sqrt{3}-1, then z=x+y>31z=x+y>\sqrt{3}-1, which contradicts 31\sqrt{3}-1 being the maximum of 2{\mathcal{B}}_{2}.

Therefore, z=x+y=31z=x+y=\sqrt{3}-1 and x=y=312x=y=\frac{\sqrt{3}-1}{2}. ∎

We can now provide a concise proof of Theorem 1.6. Indeed, we will see that the main part of the proof can be summarized by the careful analysis of cases shown in Table 1 and Table 2, which we present below. However, the reader may also wish to refer to (3.1) and Remark 3.2 for an intuitive explanation of why this case analysis is stable as the parameter nn increases.

Proof of Theorem 1.6.

Assume that xyzx\leq y\leq z. We divide the proof into 4 cases:

Case 1. x,y,z2x,y,z\in{\mathcal{B}}_{2}.

This case is impossible by Remark 1.5.

Case 2. x2,12x\in{\mathcal{B}}_{2,1}\setminus{\mathcal{B}}_{2}, and y,z2y,z\in{\mathcal{B}}_{2}.

Setting x=13+Xx=\frac{1}{3+X} with X2X\in{\mathcal{B}}_{2}, we have

y+z=113+X=11+12+X2.y+z=1-\frac{1}{3+X}=\frac{1}{1+\frac{1}{2+X}}\in{\mathcal{B}}_{2}\,.

By Lemma 2.2, we obtain

y=z=312,113+X=31,y=z=\frac{\sqrt{3}-1}{2}\,,\quad 1-\frac{1}{3+X}=\sqrt{3}-1\,,

i.e.

x=13+X=23=[3,1,2¯],y=z=312=[2,1¯],\displaystyle x=\frac{1}{3+X}=2-\sqrt{3}=[3,\overline{1,2}]\,,\quad y=z=\frac{\sqrt{3}-1}{2}=[\overline{2,1}]\,, (2.7)

is the solution of x+y+z=1x+y+z=1.

Case 3. x,y2,12x,y\in{\mathcal{B}}_{2,1}\setminus{\mathcal{B}}_{2}, and z2z\in{\mathcal{B}}_{2}.

In this case, the continued fraction expansions of xx and yy both satisfy a1=3a_{1}=3, aj2a_{j}\leq 2 for all j2j\geq 2. Under these assumptions, we aim to show that

x=y=222=[3,2¯],z=21=[2¯],x=y=\frac{2-\sqrt{2}}{2}=[3,\overline{2}]\,,\quad z=\sqrt{2}-1=[\overline{2}]\,,

is the only possible solution. First, we introduce variables Xn,Yn,ZnX_{n},Y_{n},Z_{n} to represent arbitrary numbers satisfying a certain property that depends on a given nonnegative integer nn. More specifically, we will prove the following statement:

For each n0n\geq 0 , if XnI(3,(2)n+1)X_{n}\notin I(3,(2)^{n+1}) or YnI(3,(2)n+1)Y_{n}\notin I(3,(2)^{n+1}), then Zn=1XnYnZ_{n}=1-X_{n}-Y_{n} is contained in a forbidden pattern.

We divide the proof into 2 cases according to the parity of nn.

Case 3.1. nn is even.

The computations when nn is even are summarized in Table 1. There are 17 cases that must be considered for the cylinder sets of XnX_{n} and YnY_{n}.

Case Cylinder set for XnX_{n} Cylinder set for YnY_{n} Left endpoint of the forbidden pattern Right endpoint of the forbidden pattern
1 I(3,(2)n,1)I(3,(2)^{n},1) I(3,(2)n,1)I(3,(2)^{n},1) [(2)n+1,3,][(2)^{n+1},3,\infty] [(2)n+1,][(2)^{n+1},\infty]
2.1 I(3,(2)n,1,2)I(3,(2)^{n},1,2) I(3,(2)n,2,2)I(3,(2)^{n},2,2) [(2)n+1,3,][(2)^{n+1},3,\infty] [(2)n+1,3,1,][(2)^{n+1},3,1,\infty]
2.2 I(3,(2)n,1,2)I(3,(2)^{n},1,2) I(3,(2)n,2,1)I(3,(2)^{n},2,1) [(2)n+1,(2,1),12,][(2)^{n+1},(2,1),12,\infty] [(2)n+1,3,1,][(2)^{n+1},3,1,\infty]
2.3.1 I(3,(2)n,1,1,1)I(3,(2)^{n},1,1,1) I(3,(2)n,2,2,1)I(3,(2)^{n},2,2,1) [(2)n+1,3,][(2)^{n+1},3,\infty] [(2)n+1,3,2,][(2)^{n+1},3,2,\infty]
2.3.2 I(3,(2)n,1,1,1)I(3,(2)^{n},1,1,1) I(3,(2)n,2,2,2)I(3,(2)^{n},2,2,2) [(2)n+1,3,][(2)^{n+1},3,\infty] [(2)n+1,3,3,][(2)^{n+1},3,3,\infty]
2.3.3 I(3,(2)n,1,1,2)I(3,(2)^{n},1,1,2) I(3,(2)n,2,2,1)I(3,(2)^{n},2,2,1) [(2)n+1,(2,1),14,][(2)^{n+1},(2,1),14,\infty] [(2)n+1,3,10,][(2)^{n+1},3,10,\infty]
2.3.4 I(3,(2)n,1,1,2)I(3,(2)^{n},1,1,2) I(3,(2)n,2,2,2)I(3,(2)^{n},2,2,2) [(2)n+1,(2,1),10,][(2)^{n+1},(2,1),10,\infty] [(2)n+1,3,20,][(2)^{n+1},3,20,\infty]
2.4.1 I(3,(2)n,1,1,1)I(3,(2)^{n},1,1,1) I(3,(2)n,2,1,1)I(3,(2)^{n},2,1,1) [(2)n+1,(2,1),6,][(2)^{n+1},(2,1),6,\infty] [(2)n+1,3,4,][(2)^{n+1},3,4,\infty]
2.4.2 I(3,(2)n,1,1,1)I(3,(2)^{n},1,1,1) I(3,(2)n,2,1,2)I(3,(2)^{n},2,1,2) [(2)n+1,(2,1),4,][(2)^{n+1},(2,1),4,\infty] [(2)n+1,3,8,][(2)^{n+1},3,8,\infty]
2.4.3 I(3,(2)n,1,1,2)I(3,(2)^{n},1,1,2) I(3,(2)n,2,1,1)I(3,(2)^{n},2,1,1) [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty] [(2)n+1,2,1,][(2)^{n+1},2,1,\infty]
2.4.4.1.1 I(3,(2)n,1,1,2,1,1)I(3,(2)^{n},1,1,2,1,1) I(3,(2)n,2,1,2,1,1)I(3,(2)^{n},2,1,2,1,1) [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty] [(2)n+1,2,1,][(2)^{n+1},2,1,\infty]
2.4.4.1.2 I(3,(2)n,1,1,2,1,1)I(3,(2)^{n},1,1,2,1,1) I(3,(2)n,2,1,2,1,2)I(3,(2)^{n},2,1,2,1,2) [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty] [(2)n+1,2,1,][(2)^{n+1},2,1,\infty]
2.4.4.1.3 I(3,(2)n,1,1,2,1,2)I(3,(2)^{n},1,1,2,1,2) I(3,(2)n,2,1,2,1,2)I(3,(2)^{n},2,1,2,1,2) [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty] [(2)n+1,2,1,][(2)^{n+1},2,1,\infty]
2.4.4.1.4 I(3,(2)n,1,1,2,1,2)I(3,(2)^{n},1,1,2,1,2) I(3,(2)n,2,1,2,1,1)I(3,(2)^{n},2,1,2,1,1) [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty] [(2)n+1,2,1,][(2)^{n+1},2,1,\infty]
2.4.4.2 I(3,(2)n,1,1,2,1)I(3,(2)^{n},1,1,2,1) I(3,(2)n,2,1,2,2)I(3,(2)^{n},2,1,2,2) [(2)n+1,(2,1)2,20,][(2)^{n+1},(2,1)^{2},20,\infty] [(2)n+1,2,1,][(2)^{n+1},2,1,\infty]
2.4.4.3 I(3,(2)n,1,1,2,2)I(3,(2)^{n},1,1,2,2) I(3,(2)n,2,1,2,1)I(3,(2)^{n},2,1,2,1) [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty] [(2)n+1,2,1,][(2)^{n+1},2,1,\infty]
2.4.4.4 I(3,(2)n,1,1,2,2)I(3,(2)^{n},1,1,2,2) I(3,(2)n,2,1,2,2)I(3,(2)^{n},2,1,2,2) [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty] [(2)n+1,2,1,][(2)^{n+1},2,1,\infty]
Table 1. Case analysis showing the forbidden patterns containing Zn=1XnYnZ_{n}=1-X_{n}-Y_{n} when nn is even.

The computations are lengthy and we only detail Case 2.1 of Table 1 in this paper.

To prove the result for Case 2.1 in Table 1, assume that

XnI(3,(2)n,1,2),YnI(3,(2)n,2,2).X_{n}\in I(3,(2)^{n},1,2)\,,\quad Y_{n}\in I(3,(2)^{n},2,2)\,.

Let

An=122+1219219+62+17(1+2)2n+4,Bn=122+10+21+527(1+2)2n+5,A_{n}=1-\tfrac{\sqrt{2}}{2}+\tfrac{12-19\sqrt{2}}{-19+6\sqrt{2}+17(1+\sqrt{2})^{2n+4}}\,,\quad B_{n}=1-\tfrac{\sqrt{2}}{2}+\tfrac{10+\sqrt{2}}{1+5\sqrt{2}-7(1+\sqrt{2})^{2n+5}}\,,

and

Cn=122+2(1+2)2n+8+1,Dn=122+2(1+2)2n+8+1.C_{n}=1-\tfrac{\sqrt{2}}{2}+\tfrac{\sqrt{2}}{-(1+\sqrt{2})^{2n+8}+1}\,,\quad D_{n}=1-\tfrac{\sqrt{2}}{2}+\tfrac{\sqrt{2}}{(1+\sqrt{2})^{2n+8}+1}\,.

By calculating, we get

I(3,(2)n,1,2)=(An,Bn]=122+(1219219+62+17(1+2)2n+4,10+21+527(1+2)2n+5],I(3,(2)^{n},1,2)=(A_{n},B_{n}]=1-\tfrac{\sqrt{2}}{2}+\left(\tfrac{12-19\sqrt{2}}{-19+6\sqrt{2}+17(1+\sqrt{2})^{2n+4}},\tfrac{10+\sqrt{2}}{1+5\sqrt{2}-7(1+\sqrt{2})^{2n+5}}\right]\,,
I(3,(2)n,2,2)=(Cn,Dn]=122+(2(1+2)2n+8+1,2(1+2)2n+8+1].\ I(3,(2)^{n},2,2)=(C_{n},D_{n}]=1-\tfrac{\sqrt{2}}{2}+\left(\tfrac{\sqrt{2}}{-(1+\sqrt{2})^{2n+8}+1},\tfrac{\sqrt{2}}{(1+\sqrt{2})^{2n+8}+1}\right]\,.

We claim that

Zn=1XnYn[[(2)n+1,3,],[(2)n+1,3,1,]].\displaystyle Z_{n}=1-X_{n}-Y_{n}\in\left[[(2)^{n+1},3,\infty]\,,[(2)^{n+1},3,1,\infty]\right]\,.

Since n+1n+1 is odd, by Lemma 2.1, this implies that the bounds on ZnZ_{n} are contained in a forbidden pattern. Indeed,

Zn=1XnYn[1BnDn,1AnCn),Z_{n}=1-X_{n}-Y_{n}\in[1-B_{n}-D_{n},1-A_{n}-C_{n})\,,

by direct computation, we get

1BnDn=2110+21+527(1+2)2n+52(1+2)2n+8+1,1-B_{n}-D_{n}=\sqrt{2}-1-\tfrac{10+\sqrt{2}}{1+5\sqrt{2}-7(1+\sqrt{2})^{2n+5}}-\tfrac{\sqrt{2}}{(1+\sqrt{2})^{2n+8}+1}\,,
1AnCn=211219219+62+17(1+2)2n+42(1+2)2n+8+1.1-A_{n}-C_{n}=\sqrt{2}-1-\tfrac{12-19\sqrt{2}}{-19+6\sqrt{2}+17(1+\sqrt{2})^{2n+4}}-\tfrac{\sqrt{2}}{-(1+\sqrt{2})^{2n+8}+1}\,.

By assumption nn is even, so

(1BnDn)[(2)n+1,3,]\displaystyle\ \ \ \ (1-B_{n}-D_{n})-[(2)^{n+1},3,\infty]
=2110+21+527(1+2)2n+52(1+2)2n+8+1(3+22)n+2+1(12)(3+22)n+2+1+2\displaystyle=\sqrt{2}-1-\tfrac{10+\sqrt{2}}{1+5\sqrt{2}-7(1+\sqrt{2})^{2n+5}}-\tfrac{\sqrt{2}}{(1+\sqrt{2})^{2n+8}+1}-\tfrac{(-3+2\sqrt{2})^{n+2}+1}{(1-\sqrt{2})(-3+2\sqrt{2})^{n+2}+1+\sqrt{2}}
=(1+2)n(24+162)(12)n(24+162)((12)n+3(1+2)n+3)(10+(221)(12)2n+6(22+1)(1+2)2n+6),\displaystyle=\tfrac{(1+\sqrt{2})^{n}(24+16\sqrt{2})-(1-\sqrt{2})^{n}(-24+16\sqrt{2})}{\left(-(1-\sqrt{2})^{n+3}-(1+\sqrt{2})^{n+3}\right)\left(10+(2\sqrt{2}-1)(1-\sqrt{2})^{2n+6}-(2\sqrt{2}+1)(1+\sqrt{2})^{2n+6}\right)}\,,

is positive. We can see this by checking that the numerator and the denominator are both positive. Indeed, since |1+2|>|12|\left|1+\sqrt{2}\right|>\left|1-\sqrt{2}\right| and |24+162|>|24+162|\left|24+16\sqrt{2}\right|>\left|-24+16\sqrt{2}\right|, the numerator is positive. Similarly, the first term in the denominator (12)n+3(1+2)n+3-(1-\sqrt{2})^{n+3}-(1+\sqrt{2})^{n+3} is negative since |12|<|1+2|\left|1-\sqrt{2}\right|<\left|1+\sqrt{2}\right|. Now, since |221|<|22+1|\left|2\sqrt{2}-1\right|<\left|2\sqrt{2}+1\right| and |12|<|1+2|\left|1-\sqrt{2}\right|<\left|1+\sqrt{2}\right|, the second term in the denominator

10+(221)(12)2n+6(22+1)(1+2)2n+6,10+(2\sqrt{2}-1)(1-\sqrt{2})^{2n+6}-(2\sqrt{2}+1)(1+\sqrt{2})^{2n+6}\,,

is negative, so the denominator is positive. Therefore, the quotient is positive, as desired.

Next, we verify that

[(2)n+1,3,1,](1AnCn)\displaystyle\ \ \ \ \ [(2)^{n+1},3,1,\infty]-(1-A_{n}-C_{n})
=17(9+42)(3+22)n+2+117(152)(3+22)n+2+1+2(211219219+62+17(1+2)2n+42(1+2)2n+8+1)\displaystyle=\tfrac{\frac{1}{7}(9+4\sqrt{2})(-3+2\sqrt{2})^{n+2}+1}{\frac{1}{7}(1-5\sqrt{2})(-3+2\sqrt{2})^{n+2}+1+\sqrt{2}}-\left(\sqrt{2}-1-\tfrac{12-19\sqrt{2}}{-19+6\sqrt{2}+17(1+\sqrt{2})^{2n+4}}-\tfrac{\sqrt{2}}{-(1+\sqrt{2})^{2n+8}+1}\right)
=(1+2)n(72+602)(12)n(72+602)((12)n+3(4+2)+(1+2)n+3(42))(28+(12)2n+6(62)+(1+2)2n+6(6+2)),\displaystyle=\tfrac{(1+\sqrt{2})^{n}(72+60\sqrt{2})-(1-\sqrt{2})^{n}(-72+60\sqrt{2})}{\left((1-\sqrt{2})^{n+3}(4+\sqrt{2})+(1+\sqrt{2})^{n+3}(4-\sqrt{2})\right)\left(-28+(1-\sqrt{2})^{2n+6}(6-\sqrt{2})+(1+\sqrt{2})^{2n+6}(6+\sqrt{2})\right)}\,,

is positive. As before, we can see this by checking that the numerator and the denominator are both positive. This time, we have |1+2|>|12|\left|1+\sqrt{2}\right|>\left|1-\sqrt{2}\right| and |72+602|>|72602|\left|72+60\sqrt{2}\right|>\left|72-60\sqrt{2}\right|, so the numerator is positive. Similarly, it is easy to check that the first term and the second term in the denominator are positive, so the denominator is positive. Therefore, the quotient is positive, as desired. Thus, we obtain that

Zn=1XnYn[[(2)n+1,3,],[(2)n+1,3,1,]],Z_{n}=1-X_{n}-Y_{n}\in\left[[(2)^{n+1},3,\infty],[(2)^{n+1},3,1,\infty]\right]\,,

which implies that the bounds on ZnZ_{n} are contained in a forbidden pattern. The other cases in Table 1 can be proven in the same way.

Case 3.2. nn is odd.

The computations of forbidden patterns containing Zn=1XnYnZ_{n}=1-X_{n}-Y_{n} when nn is odd are summarized in Table 2, where XnI(3,(2)n+1)X_{n}\notin I(3,(2)^{n+1}) or YnI(3,(2)n+1)Y_{n}\notin I(3,(2)^{n+1}). Again, there are 17 cases that must be considered. The proofs are similar to those for the even case.

Case Cylinder set for XnX_{n} Cylinder set for YnY_{n} Left endpoint of the forbidden pattern Right endpoint of the forbidden pattern
1 I(3,(2)n,1)I(3,(2)^{n},1) I(3,(2)n,1)I(3,(2)^{n},1) [(2)n+1,][(2)^{n+1},\infty] [(2)n+1,3,][(2)^{n+1},3,\infty]
2.1 I(3,(2)n,1,2)I(3,(2)^{n},1,2) I(3,(2)n,2,2)I(3,(2)^{n},2,2) [(2)n+1,3,1,][(2)^{n+1},3,1,\infty] [(2)n+1,3,][(2)^{n+1},3,\infty]
2.2 I(3,(2)n,1,2)I(3,(2)^{n},1,2) I(3,(2)n,2,1)I(3,(2)^{n},2,1) [(2)n+1,3,1,][(2)^{n+1},3,1,\infty] [(2)n+1,(2,1),12,][(2)^{n+1},(2,1),12,\infty]
2.3.1 I(3,(2)n,1,1,1)I(3,(2)^{n},1,1,1) I(3,(2)n,2,2,1)I(3,(2)^{n},2,2,1) [(2)n+1,3,2,][(2)^{n+1},3,2,\infty] [(2)n+1,3,][(2)^{n+1},3,\infty]
2.3.2 I(3,(2)n,1,1,1)I(3,(2)^{n},1,1,1) I(3,(2)n,2,2,2)I(3,(2)^{n},2,2,2) [(2)n+1,3,3,][(2)^{n+1},3,3,\infty] [(2)n+1,3,][(2)^{n+1},3,\infty]
2.3.3 I(3,(2)n,1,1,2)I(3,(2)^{n},1,1,2) I(3,(2)n,2,2,1)I(3,(2)^{n},2,2,1) [(2)n+1,3,10,][(2)^{n+1},3,10,\infty] [(2)n+1,(2,1),14,][(2)^{n+1},(2,1),14,\infty]
2.3.4 I(3,(2)n,1,1,2)I(3,(2)^{n},1,1,2) I(3,(2)n,2,2,2)I(3,(2)^{n},2,2,2) [(2)n+1,3,20,][(2)^{n+1},3,20,\infty] [(2)n+1,(2,1),10,][(2)^{n+1},(2,1),10,\infty]
2.4.1 I(3,(2)n,1,1,1)I(3,(2)^{n},1,1,1) I(3,(2)n,2,1,1)I(3,(2)^{n},2,1,1) [(2)n+1,3,4,][(2)^{n+1},3,4,\infty] [(2)n+1,(2,1),6,][(2)^{n+1},(2,1),6,\infty]
2.4.2 I(3,(2)n,1,1,1)I(3,(2)^{n},1,1,1) I(3,(2)n,2,1,2)I(3,(2)^{n},2,1,2) [(2)n+1,3,8,][(2)^{n+1},3,8,\infty] [(2)n+1,(2,1),4,][(2)^{n+1},(2,1),4,\infty]
2.4.3 I(3,(2)n,1,1,2)I(3,(2)^{n},1,1,2) I(3,(2)n,2,1,1)I(3,(2)^{n},2,1,1) [(2)n+1,2,1,][(2)^{n+1},2,1,\infty] [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty]
2.4.4.1.1 I(3,(2)n,1,1,2,1,1)I(3,(2)^{n},1,1,2,1,1) I(3,(2)n,2,1,2,1,1)I(3,(2)^{n},2,1,2,1,1) [(2)n+1,2,1,][(2)^{n+1},2,1,\infty] [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty]
2.4.4.1.2 I(3,(2)n,1,1,2,1,1)I(3,(2)^{n},1,1,2,1,1) I(3,(2)n,2,1,2,1,2)I(3,(2)^{n},2,1,2,1,2) [(2)n+1,2,1,][(2)^{n+1},2,1,\infty] [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty]
2.4.4.1.3 I(3,(2)n,1,1,2,1,2)I(3,(2)^{n},1,1,2,1,2) I(3,(2)n,2,1,2,1,2)I(3,(2)^{n},2,1,2,1,2) [(2)n+1,2,1,][(2)^{n+1},2,1,\infty] [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty]
2.4.4.1.4 I(3,(2)n,1,1,2,1,2)I(3,(2)^{n},1,1,2,1,2) I(3,(2)n,2,1,2,1,1)I(3,(2)^{n},2,1,2,1,1) [(2)n+1,2,1,][(2)^{n+1},2,1,\infty] [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty]
2.4.4.2 I(3,(2)n,1,1,2,1)I(3,(2)^{n},1,1,2,1) I(3,(2)n,2,1,2,2)I(3,(2)^{n},2,1,2,2) [(2)n+1,2,1,][(2)^{n+1},2,1,\infty] [(2)n+1,(2,1)2,20,][(2)^{n+1},(2,1)^{2},20,\infty]
2.4.4.3 I(3,(2)n,1,1,2,2)I(3,(2)^{n},1,1,2,2) I(3,(2)n,2,1,2,1)I(3,(2)^{n},2,1,2,1) [(2)n+1,2,1,][(2)^{n+1},2,1,\infty] [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty]
2.4.4.4 I(3,(2)n,1,1,2,2)I(3,(2)^{n},1,1,2,2) I(3,(2)n,2,1,2,2)I(3,(2)^{n},2,1,2,2) [(2)n+1,2,1,][(2)^{n+1},2,1,\infty] [(2)n+1,(2,1),3,][(2)^{n+1},(2,1),3,\infty]
Table 2. Case analysis showing the forbidden patterns containing Zn=1XnYnZ_{n}=1-X_{n}-Y_{n} when nn is odd.

Immediately, from Table 1 and Table 2, we see that

XnI(3,(2)n,1),YnI(3,(2)n,1),\displaystyle X_{n}\in I(3,(2)^{n},1)\,,\quad Y_{n}\in I(3,(2)^{n},1)\,,

is impossible by Case 1. Together, Cases 2.3.1 to 2.3.4 show that

XnI(3,(2)n,1,1),YnI(3,(2)n,2,2),\displaystyle X_{n}\in I(3,(2)^{n},1,1)\,,\quad Y_{n}\in I(3,(2)^{n},2,2)\,, (2.8)

is impossible. Next, Cases 2.4.4.1.1 to 2.4.4.1.4 show that it is impossible to have XnI(3,(2)n,1,1,2,1)X_{n}\in I(3,(2)^{n},1,1,2,1) and YnI(3,(2)n,2,1,2,1)Y_{n}\in I(3,(2)^{n},2,1,2,1). By this and Cases 2.4.4.2 to 2.4.4.4, we get that it is impossible to have XnI(3,(2)n,1,1,2)X_{n}\in I(3,(2)^{n},1,1,2) and YnI(3,(2)n,2,1,2)Y_{n}\in I(3,(2)^{n},2,1,2). This, together with Cases 2.4.1 to 2.4.3, shows that

XnI(3,(2)n,1,1),YnI(3,(2)n,2,1),\displaystyle X_{n}\in I(3,(2)^{n},1,1)\,,\quad Y_{n}\in I(3,(2)^{n},2,1)\,, (2.9)

is impossible. Next, from Case 2.1, Case 2.2, (2.8), and (2.9), we obtain that

XnI(3,(2)n,1),YnI(3,(2)n,2),\displaystyle X_{n}\in I(3,(2)^{n},1)\,,\quad Y_{n}\in I(3,(2)^{n},2)\,,

is impossible. This analysis of cases shows that any solution of Xn+Yn+Zn=1X_{n}+Y_{n}+Z_{n}=1 must satisfy

Xn,YnI(3,(2)n+1).X_{n}\,,Y_{n}\in I(3,(2)^{n+1})\,.

Therefore,

x=y=222=[3,2¯],z=21=[2¯],\displaystyle x=y=\frac{2-\sqrt{2}}{2}=[3,\overline{2}]\,,\quad z=\sqrt{2}-1=[\overline{2}]\,, (2.10)

is the only possible solution of x+y+z=1x+y+z=1 for this case.

Case 4. x,y,z2,12x,y,z\in{\mathcal{B}}_{2,1}\setminus{\mathcal{B}}_{2}.

We claim that this case is impossible. In fact, I(3)=[14,13)I(3)=[\frac{1}{4},\frac{1}{3}), so x+y+z<1x+y+z<1, which is a contradiction. Therefore, by (2.7) and (2.10), the theorem is proven. ∎

Proof of Theorem 1.7.

Observe that x,y,z2,1x,y,z\in{\mathcal{B}}_{2,1} satisfy the equality x+y+z=1x+y+z=1 if and only if the three equalities

x+y=1z,x+z=1y,y+z=1x,x+y=1-z\,,\quad x+z=1-y\,,\quad y+z=1-x\,, (2.11)

are also satisfied. Moreover, by Corollary 1.3, the numbers 1z1-z, 1y1-y, and 1x1-x must also be in 2,1{\mathcal{B}}_{2,1}. Next, recall from Theorem 1.6 that

x=23=[3,1,2¯],y=z=312=[2,1¯],x=2-\sqrt{3}=[3,\overline{1,2}]\,,\quad y=z=\frac{\sqrt{3}-1}{2}=[\overline{2,1}]\,, (2.12)

and

x=y=222=[3,2¯],z=21=[2¯],x=y=\frac{2-\sqrt{2}}{2}=[3,\overline{2}]\,,\quad z=\sqrt{2}-1=[\overline{2}]\,, (2.13)

are the only solutions of the equality x+y+z=1,(x,y,z2,1,xyz)x+y+z=1\,,\ (x,y,z\in{\mathcal{B}}_{2,1}\,,\ x\leq y\leq z).

In (2.12), the solution of x+y+z=1x+y+z=1 happens to have y=zy=z, so (2.12) provides two solutions of our target equality due to (2.11). Specifically, we get that

x=23=[3,1,2¯],y=312=[2,1¯],z=332=[1,1,1,2,1¯],x=2-\sqrt{3}=[3,\overline{1,2}]\,,\quad y=\frac{\sqrt{3}-1}{2}=[\overline{2,1}]\,,\quad z=\frac{3-\sqrt{3}}{2}=[1,1,1,\overline{2,1}]\,,

and

x=y=312=[2,1¯],z=31=[1,2¯],x=y=\frac{\sqrt{3}-1}{2}=[\overline{2,1}]\,,\quad z=\sqrt{3}-1=[\overline{1,2}]\,,

are both solutions of the equality x+y=z,(x,y,z2,1,xy)x+y=z\,,\ (x,y,z\in{\mathcal{B}}_{2,1}\,,x\leq y).

In (2.13), the solution of x+y+z=1x+y+z=1 happens to have x=yx=y, so (2.13) provides two more solutions of our target equality due to (2.11). Specifically, we get that

x=y=222=[3,2¯],z=22=[1,1,2¯],x=y=\frac{2-\sqrt{2}}{2}=[3,\overline{2}]\,,\quad z=2-\sqrt{2}=[1,1,\overline{2}]\,,

and

x=222=[3,2¯],y=21=[2¯],z=22=[1,2¯],x=\frac{2-\sqrt{2}}{2}=[3,\overline{2}]\,,\quad y=\sqrt{2}-1=[\overline{2}]\,,\quad z=\frac{\sqrt{2}}{2}=[1,\overline{2}]\,,

are also solutions of the equality x+y=z,(x,y,z2,1,xy)x+y=z\,,\ (x,y,z\in{\mathcal{B}}_{2,1}\,,x\leq y).

Finally, we know that these four solutions are the only possibilities because any additional solution to the equality x+y=z,(x,y,z2,1,xy)x+y=z\,,\ (x,y,z\in{\mathcal{B}}_{2,1}\,,x\leq y) would produce an additional solution to x+y+z=1,(xyz)x+y+z=1\,,\ (x\leq y\leq z), which is impossible by Theorem 1.6. ∎

Remark 2.3.

Observe that Table 2 can be obtained from Table 1 by exchanging the left and the right endpoints of the forbidden patterns in the second-last and last columns.

3. Proof of Theorem 1.8

Proof.

By Theorem 1.6, we know that there are exactly two solutions of the equality x+y+z=1x+y+z=1 under the restrictions x,y,z2,1x,y,z\in{\mathcal{B}}_{2,1} and xyzx\leq y\leq z. Starting from the second solution

x=y=222=[3,2¯],z=21=[2¯],x=y=\frac{2-\sqrt{2}}{2}=[3,\overline{2}],\ z=\sqrt{2}-1=[\overline{2}]\,,

we can construct further explicit solutions of the equation x+y+z=1x+y+z=1 under the weaker restrictions x,y,z2x,y,z\in{\mathcal{B}}_{2}^{*} and x,y,z3x,y,z\in{\mathcal{B}}_{3}. We do this by making certain insertions into the continued fraction expansions of xx, yy, and zz.

Consider the result of inserting a 2 after the number 3 in the continued fraction expansions of xx and yy, and inserting a 2 foremost in the continued fraction expansion of zz. This produces new numbers XX, YY, ZZ that satisfy

X=13+11x1,Y=13+11y1,Z=12+z.X=\cfrac{1}{3+\cfrac{1}{\cfrac{1}{x}-1}}\,,\quad Y=\cfrac{1}{3+\cfrac{1}{\cfrac{1}{y}-1}}\,,\quad Z=\cfrac{1}{2+z}\,.

From these expressions, we obtain the equality

1XYZ=(xy)2(32x)(32y)(3xy),1-X-Y-Z=\frac{(x-y)^{2}}{(3-2x)(3-2y)(3-x-y)}\,, (3.1)

which implies that X+Y+Z=1X+Y+Z=1 because x=yx=y.

Similarly, consider a different type of insertion where we insert 3,1,33,1,3 after the number 33 in the continued fraction expansions of xx and yy, and 1,1,2,1,11,1,2,1,1 after the number 22 in the continued fraction expansion of zz. In this case, we get new numbers XX, YY, and ZZ that satisfy

X=13+13+11+x,Y=13+13+11+y,Z=12+11+11+12+11+11z1.X=\cfrac{1}{3+\cfrac{1}{3+\cfrac{1}{1+x}}}\,,\quad Y=\cfrac{1}{3+\cfrac{1}{3+\cfrac{1}{1+y}}}\,,\quad Z=\cfrac{1}{2+\cfrac{1}{1+\cfrac{1}{1+\cfrac{1}{2+\cfrac{1}{1+\cfrac{1}{\cfrac{1}{z}-1}}}}}}\,.

This gives us the equality

1XYZ=5(xy)2(10x+13)(10y+13)(5x+5y+13),1-X-Y-Z=\frac{-5(x-y)^{2}}{(10x+13)(10y+13)(5x+5y+13)}\,, (3.2)

which again implies that X+Y+Z=1X+Y+Z=1 because x=yx=y.

Therefore, there are at least two different types of insertions that result in further solutions of the equality. Moreover, S={2,11211}S=\{2,11211\} is a code, i.e., any word generated by SS can be uniquely decomposed into a word over SS (see [12, Chapter 1] for a definition). From this observation, we immediately get that there are infinitely many solutions of the equality for x,y,z2x,y,z\in{\mathcal{B}}_{2}^{*}, since 2=j=12,j{\mathcal{B}}_{2}^{*}=\bigcup_{j=1}^{\infty}{\mathcal{B}}_{2,j}. Furthermore, we obtain uncountably many explicit solutions of the equality for x,y,z3x,y,z\in{\mathcal{B}}_{3} by this method. ∎

Remark 3.1.

We can also prove Theorem 1.8 by starting from the first solution of Theorem 1.6 and using the same method with a small modification to the insertions.

Remark 3.2.

By the formula (3.1), we can reprove Theorem 1.6 by induction. The right side of (3.1) gives the error term after the number 22 is inserted into the continued fraction expansions of XnX_{n}, YnY_{n}, and ZnZ_{n} in Tables 1 and 2. In particular, this error term is small enough that the number of cases to consider is always 17.

4. Construction of Delone sets by badly approximable triangles

In this section, we construct Delone sets from tilings of the plane by triangles involving angles α\alpha, β\beta, γ\gamma, where α+β+γ=π\alpha+\beta+\gamma=\pi. In the general case when α\alpha, β\beta, γ\gamma are arbitrary, we have a subdivision rule for a scalene triangle with angles α\alpha, β\beta, γ\gamma and an isosceles triangle with angles γ\gamma, γ\gamma, π2γ\pi-2\gamma, as illustrated in Figure 1.

Refer to caption
Figure 1. Subdivision rule for triangles with angles α\alpha, β\beta, γ\gamma. The triangle on the left is scalene, and the triangle on the right is isosceles. In this illustration, we have α=π3\alpha=\frac{\pi}{3}, β=π4\beta=\frac{\pi}{4}, γ=5π12\gamma=\frac{5\pi}{12}, but any solution of α+β+γ=π\alpha+\beta+\gamma=\pi can be used.

Our objective is to obtain Delone sets associated with the unique solutions to the equality x+y+z=1(x,y,z2,1,xyz)x+y+z=1\ (x,y,z\in{\mathcal{B}}_{2,1},\ x\leq y\leq z) found in Theorem 1.6:

x=23,y=z=312,x=2-\sqrt{3}\,,\quad y=z=\frac{\sqrt{3}-1}{2}\,,

and

x=y=222,z=21.x=y=\frac{2-\sqrt{2}}{2}\,,\quad z=\sqrt{2}-1\,.

For the first solution, by choosing

α=(23)π,β=γ=(31)π2,\alpha=(2-\sqrt{3})\pi\,,\quad\beta=\gamma=\frac{(\sqrt{3}-1)\pi}{2}\,, (4.1)

the subdivision rule in Figure 1 reduces to a subdivision rule involving only the isosceles triangle with angles α\alpha and β=γ\beta=\gamma as shown in Figure 2.

Refer to caption
Figure 2. Subdivision rule for the isosceles triangle with optimal badly approximable angles α\alpha and β=γ\beta=\gamma as in (4.1).

Similarly, for the second solution, by choosing

α=(21)π,β=γ=(22)π2,\alpha=(\sqrt{2}-1)\pi\,,\quad\beta=\gamma=\frac{(2-\sqrt{2})\pi}{2}\,, (4.2)

we again get a subdivision rule involving only an isosceles triangle, exactly as in Figure 2 except with different values for α\alpha and β\beta.

4.1. Delone sets and the Chabauty–Fell topology

We restrict our attention to 2{\mathbb{R}}^{2}. Throughout, we denote the Euclidean norm on 2{\mathbb{R}}^{2} by \|\cdot\|, and we write B(x,r)B(x,r) to denote the open ball of radius rr centered at xx, i.e. B(x,r)={y2:yx<r}B(x,r)=\{y\in{\mathbb{R}}^{2}\,:\,\|y-x\|<r\}. Similarly, we write B(x,r)¯\overline{B(x,r)} for the closed ball, i.e. B(x,r)¯={y2:yxr}\overline{B(x,r)}=\{y\in{\mathbb{R}}^{2}\,:\,\|y-x\|\leq r\}. We begin by recalling the definition of a Delone set.

Definition 4.1.

Let Λ\Lambda be a closed subset of X2X\subseteq{\mathbb{R}}^{2}.

  1. (i)

    If there exists an r>0r>0 such that for any xXx\in X, card(B(x,r)Λ)1\text{card}(B(x,r)\cap\Lambda)\leq 1, then Λ\Lambda is rr-uniformly discrete in XX.

  2. (ii)

    If there exists an R>0R>0 such that for any xXx\in X, B(x,R)¯Λ\overline{B(x,R)}\cap\Lambda\neq\emptyset, then Λ\Lambda is RR-relatively dense in XX.

  3. (iii)

    We say that Λ\Lambda is a (r,R)(r,R)-Delone set in XX if Λ\Lambda is both rr-uniformly discrete in XX and RR-relatively dense in XX.

Remark 4.2.

To clarify, in the above definition, the sets B(x,r)B(x,r) and B(x,R)¯\overline{B(x,R)} denote open and closed balls in 2{\mathbb{R}}^{2}, and not open and closed balls in the relative topology for XX.

Definition 4.3.

Let X2X\subseteq{\mathbb{R}}^{2} be closed. We define the following spaces of point sets:

  1. (i)

    Denote by 2X2^{X} the set of all closed subsets of XX;

  2. (ii)

    Denote by 𝒲r,R(X){\mathcal{W}}_{r,R}(X) the set of closed subsets Λ2\Lambda\subseteq{\mathbb{R}}^{2} such that Λ\Lambda is an (r,R)(r,R)-Delone set in XX.

Remark 4.4.

If XX and YY are closed subsets of 2{\mathbb{R}}^{2} and YXY\subseteq X, then any set which is rr-uniformly discrete and RR-relatively dense in XX must also be rr-uniformly discrete and RR-relatively dense in YY. In particular, we have 𝒲r,R(X)𝒲r,R(Y){\mathcal{W}}_{r,R}(X)\subseteq{\mathcal{W}}_{r,R}(Y).

In the next section, we will construct a sequence of finite point sets and show the existence of a subsequence converging to a Delone set in the Chabauty–Fell topology [4, 6]. This topology is also commonly referred to as the Chabauty topology or the Fell topology, which are defined more generally in any topological space. In the case of locally compact groups, it is also called the local rubber topology [3]. Since we work in 2{\mathbb{R}}^{2}, the Chabauty–Fell topology is metrizable and induced by the following metric (see [18, Appendix A]):

Definition 4.5 (Chabauty–Fell Topology).

For each Λ1,Λ22X\Lambda_{1},\Lambda_{2}\in 2^{X}, define

d(Λ1,Λ2)=inf{{1}{ε>0:Λ1B(0,1ε)Λ2+B(0,ε)andΛ2B(0,1ε)Λ1+B(0,ε)}}.d(\Lambda_{1},\Lambda_{2})=\inf\ \{\{1\}\cup\{\varepsilon>0\,:\,\Lambda_{1}\cap B(0,\textstyle{\frac{1}{\varepsilon}})\subseteq\Lambda_{2}+B(0,\varepsilon)\ \text{and}\ \Lambda_{2}\cap B(0,\textstyle{\frac{1}{\varepsilon}})\subseteq\Lambda_{1}+B(0,\varepsilon)\}\}\,.

The map d:2X×2X[0,)d:2^{X}\times 2^{X}\rightarrow[0,\infty) is a metric on 2X2^{X} inducing the Chabauty–Fell topology.

Remark 4.6.

It has long been known that the space 2X2^{X} is compact in the Fell topology [6]. Furthermore, it is easy to show that the space 𝒲r,R(X){\mathcal{W}}_{r,R}(X) is also compact in the Fell topology. As we will use this fact, we give a proof for X=2X={\mathbb{R}}^{2} in Appendix A.

We will deduce the existence of a subsequence converging to a Delone set using the compactness of 𝒲r,R(2)\mathcal{W}_{r,R}({\mathbb{R}}^{2}); however, our sequence will not be contained in 𝒲r,R(2)\mathcal{W}_{r,R}({\mathbb{R}}^{2}) because no finite set is relatively dense in 2{\mathbb{R}}^{2}. Thus, we will use the following easy observation about the Chabauty–Fell topology:

Proposition 4.7.

Let {Λn}n1\{\Lambda_{n}\}_{n\geq 1} be a sequence in 2X2^{X} and Λ2X\Lambda\in 2^{X}. Let {Rn}n1\{R_{n}\}_{n\geq 1} be a sequence of positive real numbers with limnRn=\lim_{n\rightarrow\infty}R_{n}=\infty. Then Λn\Lambda_{n} converges to Λ\Lambda if and only if ΛnB(0,Rn)\Lambda_{n}\cap B(0,R_{n}) converges to Λ\Lambda in the Chabauty–Fell topology.

Proof.

First, assume that Λn\Lambda_{n} converges to Λ\Lambda in the Chabauty–Fell topology. Then, for any ε>0\varepsilon>0, there exists a constant N1N_{1} such that for any nN1n\geq N_{1}, we have d(Λn,Λ)<εd(\Lambda_{n},\Lambda)<\varepsilon. That is,

ΛnB(0,1ε)Λ+B(0,ε),\Lambda_{n}\cap B(0,\tfrac{1}{\varepsilon})\subseteq\Lambda+B(0,\varepsilon)\,, (4.3)

and

ΛB(0,1ε)Λn+B(0,ε).\Lambda\cap B(0,\tfrac{1}{\varepsilon})\subseteq\Lambda_{n}+B(0,\varepsilon)\,. (4.4)

For the above ε\varepsilon, there must exist a constant N2N_{2} such that for any nN2n\geq N_{2}, Rn>1ε+εR_{n}>\tfrac{1}{\varepsilon}+\varepsilon. Let M=max{N1,N2}M=\max\{N_{1},N_{2}\}. Then by (4.3), we have

ΛnB(0,Rn)B(0,1ε)=ΛnB(0,1ε)Λ+B(0,ε)nM.\Lambda_{n}\cap B(0,R_{n})\cap B(0,\tfrac{1}{\varepsilon})=\Lambda_{n}\cap B(0,\tfrac{1}{\varepsilon})\subseteq\Lambda+B(0,\varepsilon)\quad\forall n\geq M\,. (4.5)

Furthermore, we get

ΛB(0,1ε)ΛnB(0,Rn)+B(0,ε).\Lambda\cap B(0,\tfrac{1}{\varepsilon})\subseteq\Lambda_{n}\cap B(0,R_{n})+B(0,\varepsilon)\,. (4.6)

Next, let xΛB(0,1ε)x\in\Lambda\cap B(0,\tfrac{1}{\varepsilon}). By (4.4), we have xΛn+B(0,ε)x\in\Lambda_{n}+B(0,\varepsilon). Thus, there exists some yΛny\in\Lambda_{n} and some zB(0,ε)z\in B(0,\varepsilon) such that x=y+zx=y+z. Since Rn>1ε+εR_{n}>\tfrac{1}{\varepsilon}+\varepsilon and xB(0,1ε)x\in B(0,\tfrac{1}{\varepsilon}) we have

yx+xy=x+z<1ε+ε<Rn,\|y\|\leq\|x\|+\|x-y\|=\|x\|+\|z\|<\frac{1}{\varepsilon}+\varepsilon<R_{n}\,,

so yΛnB(0,Rn)y\in\Lambda_{n}\cap B(0,R_{n}). In particular, we have x=y+zΛnB(0,Rn)+B(0,εx=y+z\in\Lambda_{n}\cap B(0,R_{n})+B(0,\varepsilon).

By (4.5) and (4.6), we have shown that d(ΛnB(0,Rn),Λ)<εd(\Lambda_{n}\cap B(0,R_{n}),\Lambda)<\varepsilon for all nMn\geq M, so ΛnB(0,Rn)\Lambda_{n}\cap B(0,R_{n}) converges to Λ\Lambda in the Chabauty–Fell topology.

Conversely, suppose that ΛnB(0,Rn)\Lambda_{n}\cap B(0,R_{n}) converges to Λ\Lambda in the Chabauty–Fell topology. For any ε>0\varepsilon>0, there exists a constant N1N_{1} such that for any nN1n\geq N_{1}, we have d(ΛnB(0,Rn),Λ)<εd(\Lambda_{n}\cap B(0,R_{n}),\Lambda)<\varepsilon. For the above ε\varepsilon, there must exist a constant N2N_{2} such that Rn>1εR_{n}>\tfrac{1}{\varepsilon} for any nN2n\geq N_{2}. Let M=max{N1,N2}M=\max\{N_{1},N_{2}\}. Then, for all nMn\geq M, we get

ΛnB(0,1ε)=ΛnB(0,Rn)B(0,1ε)Λ+B(0,ε),\Lambda_{n}\cap B(0,\tfrac{1}{\varepsilon})=\Lambda_{n}\cap B(0,R_{n})\cap B(0,\tfrac{1}{\varepsilon})\subseteq\Lambda+B(0,\varepsilon)\,,

and

ΛB(0,1ε)ΛnB(0,Rn)+B(0,ε)Λn+B(0,ε),\Lambda\cap B(0,\tfrac{1}{\varepsilon})\subseteq\Lambda_{n}\cap B(0,R_{n})+B(0,\varepsilon)\subseteq\Lambda_{n}+B(0,\varepsilon)\,,

so d(Λn,Λ)<εd(\Lambda_{n},\Lambda)<\varepsilon. Therefore, Λn\Lambda_{n} converges to Λ\Lambda in the Chabauty–Fell topology. ∎

In other words, the convergence of a sequence in the Chabauty–Fell topology is equivalent to the convergence of its restriction to larger and larger patches. Provided that we can extend our finite point sets to elements of 𝒲r,R(2)\mathcal{W}_{r,R}({\mathbb{R}}^{2}), we can use this fact and the compactness of 𝒲r,R(2)\mathcal{W}_{r,R}({\mathbb{R}}^{2}) to prove the existence of a Delone limit set.

4.2. Threshold method

To any subdivision rule on a finite set of tiles in 2{\mathbb{R}}^{2}, there is an associated graph-directed iterated function system (GIFS) consisting of similitudes. In this section, starting from a GIFS of this type, we construct a corresponding Delone set. In particular, starting from some initial tile, we apply the GIFS until the area of every tile is below some threshold ε>0\varepsilon>0. Once there are no tiles of area greater than ε\varepsilon, we inflate the finite patch by 1ε\frac{1}{\sqrt{\varepsilon}}. We call this an ε\varepsilon-rule, which is defined more precisely below.

4.2.1. GIFS

Let (V,Γ)(V,\Gamma) be a directed graph with vertex set VV and directed-edge set Γ\Gamma where both VV and Γ\Gamma are finite. Denote the set of edges from jj to ii by Γj,i\Gamma_{j,i} and assume that for any jVj\in V, there is at least one edge starting from vertex jj. Furthermore, assume that for each edge eΓe\in\Gamma, there is a corresponding contractive similitude ge:nng_{e}:\mathbb{R}^{n}\rightarrow\mathbb{R}^{n}. We call (ge)eΓ(g_{e})_{e\in\Gamma} a graph-directed IFS (GIFS) (see [14]). The invariant sets of this GIFS, also called graph-directed sets, are the unique non-empty compact sets (Tj)jV(T_{j})_{j\in V} satisfying

Tj=iVeΓj,ige(Ti),jV.T_{j}=\bigcup\limits_{i\in V}\bigcup\limits_{e\in\Gamma_{j,i}}g_{e}(T_{i}),\quad j\in V\,. (4.7)

Let ={T1,T2,,Tm}\mathcal{F}=\{T_{1},T_{2},\dots,T_{m}\} denote the invariant sets of a GIFS (ge)eΓ(g_{e})_{e\in\Gamma} with vertex set V={1,2,,m}V=\{1,2,\dots,m\}. We make the following additional assumptions on the GIFS:

  1. 1.

    Each tile in {\mathcal{F}} has a nonempty interior.

  2. 2.

    Each tile in {\mathcal{F}} satisfies the open set condition, i.e. each union in (4.7) has no interior-overlap.

  3. 3.

    The directed graph (V,Γ)(V,\Gamma) is strongly connected, i.e. for all i,jVi,j\in V, there is similar copy of TiT_{i} in the subdivision of TjT_{j}.

4.2.2. 𝜺\bm{\varepsilon}-rule.

For convenience, let ΣN\Sigma_{N} denote the set of edge sequences of length NN on (V,Γ)(V,\Gamma). In other words, ΣN\Sigma_{N} is the collection of sequences e1,e2,,eNΓe_{1},e_{2},\dots,e_{N}\in\Gamma such that the composition ge1ge2geNg_{e_{1}}\circ g_{e_{2}}\circ\dots\circ g_{e_{N}} is permitted by the GIFS. We iterate the GIFS starting from an initial tile TjT_{j}\in{\mathcal{F}} with the following ε\varepsilon-rule:

  1. (i)

    Fix 0<ε<10<\varepsilon<1. Given a finite sequence (e1,e2,,em(ε))Σm(ε)(e_{1},e_{2},\dots,e_{m(\varepsilon)})\in\Sigma_{m(\varepsilon)}, we continue applying the GIFS to the tile

    T=ge1ge2gem(ε)(Tj),T=g_{e_{1}}\circ g_{e_{2}}\circ\dots\circ g_{e_{m(\varepsilon)}}(T_{j})\,,

    while Area(T)>ε\text{Area}(T)>\varepsilon, and stop applying the GIFS to TT when Area(T)ε\text{Area}(T)\leq\varepsilon.

  2. (ii)

    Once the process in (i) terminates, we inflate the resulting collection of tiles by 1ε\frac{1}{\sqrt{\varepsilon}}. We denote the resulting finite patch by 𝒫ε(Tj)\mathcal{P}_{\varepsilon}(T_{j}).

Remark 4.8.

Let |ge||g_{e}^{\prime}| denote the contraction factor of the similitude geg_{e} in the GIFS. After applying the ε\varepsilon-rule, we are guaranteed to have Area(T)[a,1]\text{Area}(T)\in[a,1] for every tile T𝒫ε(Tj)T\in{\mathcal{P}}_{\varepsilon}(T_{j}), where

a=min{|ge|2:eΓ}.a=\min\{|g_{e}^{\prime}|^{2}\,:\,e\in\Gamma\}\,.

4.2.3. Associated point sets.

Our next step is to define a point set Λj(ε)\Lambda_{j}(\varepsilon) associated with the patch 𝒫ε(Tj){\mathcal{P}}_{\varepsilon}(T_{j}) by placing one point inside each tile. Since {\mathcal{F}} is a finite set, we can choose fixed constants r0,R0>0r_{0}\,,R_{0}>0 which do not depend on TjT_{j} and distinguished points λj(0)Tj\lambda_{j}^{(0)}\in T_{j} for each jVj\in V such that

B(λj(0),r0)TjB(λj(0),R0).B(\lambda_{j}^{(0)},r_{0})\subset T_{j}\subset B(\lambda_{j}^{(0)},R_{0})\,. (4.8)

Let 0<ε<10<\varepsilon<1 and TjT_{j}\in{\mathcal{F}}. Starting from λj(0)\lambda_{j}^{(0)}, we construct the elements of Λj(ε)\Lambda_{j}(\varepsilon) recursively as follows. For each application of the GIFS

Tj=iVeΓj,ige(Ti),jV,T_{j}=\bigcup\limits_{i\in V}\bigcup\limits_{e\in\Gamma_{j,i}}g_{e}(T_{i})\,,\quad j\in V\,,

in the ε\varepsilon-rule, we produce new points

λj(n)=iVeΓj,ige(λi(n1)),jV,\lambda_{j}^{(n)}=\bigcup\limits_{i\in V}\bigcup\limits_{e\in\Gamma_{j,i}}g_{e}(\lambda_{i}^{(n-1)})\,,\quad j\in V\,,

that replace the previous points λi(n1)\lambda_{i}^{(n-1)}. This process terminates when there are no further applications of the GIFS. Finally, we inflate the resulting collection of points by 1ε\frac{1}{\sqrt{\varepsilon}} to obtain the associated point sets Λj(ε)\Lambda_{j}(\varepsilon).

In other words, since any tile TT in 𝒫ε(Tj){\mathcal{P}}_{\varepsilon}(T_{j}) is similar to a unique TiT_{i}\in{\mathcal{F}}, we place exactly one point in TT via similarity at the same location as λi(0)Ti\lambda_{i}^{(0)}\in T_{i}. Though one can choose any points {λj(0)}jV\{\lambda_{j}^{(0)}\}_{j\in V} such that (4.8) holds, for simplicity we choose the centroid of each tile. In this case, Λj(ε)\Lambda_{j}(\varepsilon) is simply the set of centroids of the tiles in 𝒫ε(Tj){\mathcal{P}}_{\varepsilon}(T_{j}). Furthermore, we introduce the additional assumption that

min{Area(Tj):Tj}=1,max{Area(Tj):Tj}=S1,\displaystyle\min\{\text{Area}(T_{j})\,:\,T_{j}\in{\mathcal{F}}\}=1,\quad\max\{\text{Area}(T_{j})\,:\,T_{j}\in{\mathcal{F}}\}=S\geq 1\,, (4.9)

as this will simplify subsequent proofs. The value SS is related to the GIFS (ge)eΓ(g_{e})_{e\in\Gamma}; however, one can easily modify a given GIFS to satisfy (4.9) by simultaneously enlarging or shrinking all tiles TjT_{j} by a fixed similitude.

4.2.4. Existence of a Delone limit set

Next, we consider a decreasing sequence {εn}n1\{\varepsilon_{n}\}_{n\geq 1} in (0,1)(0,1) and show that the corresponding sequence of point sets {Λj(εn)}n1\{\Lambda_{j}(\varepsilon_{n})\}_{n\geq 1} has a subsequence converging to a Delone set in the Chabauty–Fell topology.

Lemma 4.9.

For any decreasing sequence {εn}n1\{\varepsilon_{n}\}_{n\geq 1} in (0,1)(0,1) with limnεn=0\lim_{n\rightarrow\infty}\varepsilon_{n}=0, there exists a sequence {Kn}n1\{K_{n}\}_{n\geq 1} of compact sets such that

  1. (i)

    KnKn+1K_{n}\subseteq K_{n+1} for all n1n\geq 1,

  2. (ii)

    n1Kn=2\cup_{n\geq 1}K_{n}={\mathbb{R}}^{2}, and

  3. (iii)

    Λj(εn)𝒲r,R(Kn)\Lambda_{j}(\varepsilon_{n})\in{\mathcal{W}}_{r,R}(K_{n}) for all n1n\geq 1, where r=aSr0r=\sqrt{\tfrac{a}{S}}r_{0} and R=R0R=R_{0}.

In other words, Λj(εn)\Lambda_{j}(\varepsilon_{n}) is an (r,R)(r,R)-Delone set in KnK_{n} for each n1n\geq 1.

Proof.

Recall from (4.8) that we have

B(λj(0),r0)TjB(λj(0),R0),Tj.B(\lambda_{j}^{(0)},r_{0})\subset T_{j}\subset B(\lambda_{j}^{(0)},R_{0})\,,\quad\forall\,T_{j}\in{\mathcal{F}}\,.

Given 0<εn<10<\varepsilon_{n}<1, consider an arbitrary tile T𝒫εn(Tj)T\in{\mathcal{P}}_{\varepsilon_{n}}(T_{j}). There must exist a unique finite sequence (e1,e2,,em(εn))Σm(εn)(e_{1},e_{2},\ldots,e_{m(\varepsilon_{n})})\in\Sigma_{m(\varepsilon_{n})} and one tile Ti0T_{i_{0}}\in{\mathcal{F}} such that

T=1εnge1ge2gem(εn)(Ti0).T=\tfrac{1}{\sqrt{\varepsilon_{n}}}g_{e_{1}}\circ g_{e_{2}}\circ\dots\circ g_{e_{m(\varepsilon_{n})}}(T_{i_{0}})\,.

Define xTx_{T} to be the point of Λj(εn)\Lambda_{j}(\varepsilon_{n}) that lies in TT, i.e.

xT=1εnge1ge2gem(εn)(λi0(0)).x_{T}=\tfrac{1}{\sqrt{\varepsilon_{n}}}g_{e_{1}}\circ g_{e_{2}}\circ\dots\circ g_{e_{m(\varepsilon_{n})}}(\lambda_{i_{0}}^{(0)})\,.

Let c=Area(T)c=\text{Area}(T) and A=Area(Ti0)A=\text{Area}(T_{i_{0}}). Hence, the linear scaling factor from Ti0T_{i_{0}} to TT is cA\sqrt{\frac{c}{A}}. Thus, scaling B(λi0(0),r0)B(\lambda_{i_{0}}^{(0)},r_{0}) by the linear factor cA\sqrt{\frac{c}{A}} will result in a ball of radius cAr0\sqrt{\frac{c}{A}}r_{0} that fits inside TT when centered at xTx_{T}. Hence, we have B(xT,cAr0)TB(x_{T},\sqrt{\frac{c}{A}}r_{0})\subseteq T. Similarly, we have TB(xT,cAR0)T\subseteq B(x_{T},\sqrt{\frac{c}{A}}R_{0}). Moreover, by Remark 4.8, we have ac1a\leq c\leq 1. By assumption 4.9, we get A[1,S]A\in[1,S]. From this, we obtain

B(xT,aSr0)B(xT,cAr0)TB(xT,cAR0)B(xT,R0)T𝒫εn(Tj).B(x_{T},\textstyle{\sqrt{\tfrac{a}{S}}}r_{0})\subseteq B(x_{T},\textstyle{\sqrt{\tfrac{c}{A}}}r_{0})\subseteq T\subseteq B(x_{T},\textstyle{\sqrt{\tfrac{c}{A}}}R_{0})\subseteq B(x_{T},R_{0})\quad\forall\,T\in{\mathcal{P}}_{\varepsilon_{n}}(T_{j})\,. (4.10)

Assume without loss of generality that λj(0)=0\lambda_{j}^{(0)}=0. Then, for each εn\varepsilon_{n}, we have that

Λj(εn)Kn=T𝒫εn(Tj)T.\Lambda_{j}(\varepsilon_{n})\subseteq K_{n}=\bigcup_{T\in{\mathcal{P}}_{\varepsilon_{n}}(T_{j})}T\,.

For this choice of KnK_{n}, it is easy to see that conditions (i) and (ii) are satisfied. To prove condition (iii), we must show that for every xKnx\in K_{n}, card(B(x,r)Λj(εn)1\text{card}(B(x,r)\cap\Lambda_{j}(\varepsilon_{n})\leq 1 and B(x,R)¯Λj(εn)\overline{B(x,R)}\cap\Lambda_{j}(\varepsilon_{n})\neq\emptyset, when r=aSr0r=\sqrt{\tfrac{a}{S}}r_{0} and R=R0R=R_{0}.

To this end, let xKnx\in K_{n} be arbitrary. By our choice of KnK_{n}, there exists T𝒫εn(Tj)T\in{\mathcal{P}}_{\varepsilon_{n}}(T_{j}) such that xTx\in T. First, notice that (4.10) gives us xB(xT,R)x\in B(x_{T},R), which implies that xTB(x,R)x_{T}\in B(x,R), so B(x,R)¯Λj(εn)\overline{B(x,R)}\cap\Lambda_{j}(\varepsilon_{n})\neq\emptyset holds. It remains to prove that card(B(x,r)Λj(εn))1\text{card}(B(x,r)\cap\Lambda_{j}(\varepsilon_{n}))\leq 1. We consider two cases:

Case 1. Assume that xx lies in B(xT,r)B(x_{T},r). Then xTB(x,r)x_{T}\in B(x,r). We claim that xTB(x,r)x_{T^{\prime}}\notin B(x,r) for any T𝒫εn(Tj)\TT^{\prime}\in{\mathcal{P}}_{\varepsilon_{n}}(T_{j})\backslash T. Indeed, we have

2rxTxTxTx+xxTr+xxT.2r\leq\|x_{T}-x_{T^{\prime}}\|\leq\|x_{T}-x\|+\|x-x_{T^{\prime}}\|\leq r+\|x-x_{T^{\prime}}\|\,. (4.11)

the first inequality holds since TT^{\prime} and TT are non-overlapping, and by (4.11) we have xxTr\|x-x_{T^{\prime}}\|\geq r.

Case 2. Assume that xx lies outside of B(xT,r)B(x_{T},r), i.e. xTB(x,r)x_{T}\notin B(x,r). We need to check that there can be at most one tile T𝒫εn(Tj)\TT^{\prime}\in{\mathcal{P}}_{\varepsilon_{n}}(T_{j})\backslash T such that xTB(x,r)x_{T^{\prime}}\in B(x,r). On the contrary, suppose that there exist two distinct tiles T,T′′𝒫εn(Tj)\TT^{\prime},T^{\prime\prime}\in{\mathcal{P}}_{\varepsilon_{n}}(T_{j})\backslash T with xT,xT′′B(x,r)x_{T^{\prime}},x_{T^{\prime\prime}}\in B(x,r). Since TT^{\prime} and T′′T^{\prime\prime} have no overlap, we must have xTxT′′2r\|x_{T^{\prime}}-x_{T^{\prime\prime}}\|\geq 2r. On the other hand, since xT,xT′′B(x,r)x_{T^{\prime}},x_{T^{\prime\prime}}\in B(x,r), the triangle inequality gives us

xTxT′′xTx+xxT′′<r+r=2r,\|x_{T^{\prime}}-x_{T^{\prime\prime}}\|\leq\|x_{T^{\prime}}-x\|+\|x-x_{T^{\prime\prime}}\|<r+r=2r\,,

a contradiction.

Thus, we have shown that card(B(x,r)Λj(εn))1\text{card}(B(x,r)\cap\Lambda_{j}(\varepsilon_{n}))\leq 1 and B(x,R)¯Λj(εn)\overline{B(x,R)}\cap\Lambda_{j}(\varepsilon_{n})\neq\emptyset. As xx was arbitrary, this completes the proof. ∎

Theorem 4.10.

There exists a subsequence of Λj(εn)\Lambda_{j}(\varepsilon_{n}) that converges to a (r,R)(r,R)-Delone set in 2{\mathbb{R}}^{2} in the Chabauty–Fell topology.

Proof.

By Lemma 4.9, we have Λj(εn)𝒲r,R(Kn)\Lambda_{j}(\varepsilon_{n})\subseteq\mathcal{W}_{r,R}(K_{n}), so there must exist a point set Λn𝒲r,R(2)\Lambda_{n}\in\mathcal{W}_{r,R}({\mathbb{R}}^{2}) such that ΛnKn=Λj(εn)\Lambda_{n}\cap K_{n}=\Lambda_{j}(\varepsilon_{n}). Next, since 𝒲r,R(2){\mathcal{W}}_{r,R}({\mathbb{R}}^{2}) is compact, there exists a subsequence {Λni}i1\{\Lambda_{n_{i}}\}_{i\geq 1} of {Λn}n1\{\Lambda_{n}\}_{n\geq 1} converging to some Λ𝒲r,R(2)\Lambda\in{\mathcal{W}}_{r,R}({\mathbb{R}}^{2}) in the Chabauty–Fell topology. Moreover, we have KnKn+1K_{n}\subseteq K_{n+1} for all nn and n1Kn=2\bigcup_{n\geq 1}K_{n}={\mathbb{R}}^{2}. By compactness of KniK_{n_{i}} in 2{\mathbb{R}}^{2} (in the Euclidean topology), we can pick a sequence RniR_{n_{i}} of positive real numbers such that KniB(0,Rni)K_{n_{i}}\subseteq B(0,R_{n_{i}}) for all ii. Therefore, by Proposition 4.7, we also have that ΛniB(0,Rni)\Lambda_{n_{i}}\cap B(0,R_{n_{i}}) converges to Λ\Lambda in the Chabauty–Fell topology. This proves the theorem. ∎

4.3. GIFS for arbitrary angles

Next, we consider the subdivision rule given in Figure 1 for arbitrary angles α,β,γ\alpha,\beta,\gamma. Below, we describe the GIFS associated with this subdivision rule. Then, as illustrated in Section 4.4, we can use this GIFS and the methods in Section 4.2 to produce a sequence of finite patches leading to a Delone set.

Let T1T_{1} and T2T_{2} be the scalene and isosceles triangle of unit area, respectively. We compute the GIFS for ={T1,T2}{\mathcal{F}}=\{T_{1},T_{2}\}. We use eiθe^{i\theta} to denote rotation about the origin by the angle θ\theta. Suppose that the bottom left corners of the tiles are at the origin. The contractive similitudes are as follows:

f1(x,y)=11+t2(x,y),\displaystyle f_{1}(x,y)=\tfrac{1}{1+t^{2}}(x,y)\,, (4.12)
f2(x,y)=ts(1+t2)(x,y)ei(πβ)+(a,0)+at(cosγ,sinγ),\displaystyle f_{2}(x,y)=\tfrac{t}{s(1+t^{2})}(-x,y)\cdot e^{i(\pi-\beta)}+(a,0)+at(\cos\gamma,\sin\gamma)\,,
f3(x,y)=t1+t2(x,y)eiγ+(a,0),\displaystyle f_{3}(x,y)=\tfrac{t}{1+t^{2}}(x,y)\cdot e^{i\gamma}+(a,0)\,,
f4(x,y)=Ct1+t2(x,y)eiα+(bu,0),\displaystyle f_{4}(x,y)=\tfrac{\sqrt{C}t}{1+t^{2}}(-x,y)\cdot e^{i\alpha}+(bu,0)\,,
f5(z)=Ct1+t2(x,y)ei(πα)+(bu,0)+bt(cosα,sinα),\displaystyle f_{5}(z)=\tfrac{\sqrt{C}t}{1+t^{2}}(-x,y)\cdot e^{i(\pi-\alpha)}+(bu,0)+bt(\cos\alpha,\sin\alpha)\,,
g1(x,y)=uC(st+u)(x,y)ei(πβ)+(a,0)+at(cos(γ),sin(γ)),\displaystyle g_{1}(x,y)=\tfrac{u}{\sqrt{C}(st+u)}(x,y)\cdot e^{i(\pi-\beta)}+(a,0)+at(\cos(\gamma),\sin(\gamma))\,,
g2(x,y)=ust+u(x,y),\displaystyle g_{2}(x,y)=\tfrac{u}{st+u}(x,y)\,,
g3(x,y)=stst+u(x,y)+bst2(cosγ,sinγ),\displaystyle g_{3}(x,y)=\tfrac{st}{st+u}(x,y)+bst^{2}(\cos\gamma,\sin\gamma)\,,

where

s=sinβsinγ,t=sinαsinβ,u=2st2cosγ=2sin2γsinβtanγ,C=2(1+t2)2sinαcotγt(st+u)(1+2tcosγ),s=\tfrac{\sin\beta}{\sin\gamma}\,,\quad t=\tfrac{\sin\alpha}{\sin\beta}\,,\quad u=2st^{2}\cos\gamma=\tfrac{2\sin^{2}\gamma}{\sin\beta\tan\gamma}\,,\quad C=\tfrac{2(1+t^{2})^{2}\sin\alpha\cot\gamma}{t(st+u)(1+2t\cos\gamma)}\,,

and

a=11+t22ssin(α),b=2cot(γ)st(st+u)(2tcos(γ)+1).a=\tfrac{1}{1+t^{2}}\sqrt{\tfrac{2}{s\sin(\alpha)}}\,,\quad b=2\sqrt{\tfrac{\cot(\gamma)}{st(st+u)(2t\cos(\gamma)+1)}}\,.

Then we get

T1=g1(T2)f1(T1)f2(T1)f3(T1),T_{1}=g_{1}(T_{2})\cup f_{1}(T_{1})\cup f_{2}(T_{1})\cup f_{3}(T_{1})\,,

and

T2=g2(T2)g3(T2)f4(T1)f5(T1).T_{2}=g_{2}(T_{2})\cup g_{3}(T_{2})\cup f_{4}(T_{1})\cup f_{5}(T_{1})\,.

4.4. Tilings with optimal badly approximable angles

In this section, we provide some illustrations of our construction in Section 4.3 in the specific case when α\alpha and β=γ\beta=\gamma are as in (4.1)\eqref{eq:optimal1-angles} and (4.2). First, in Figure 3, we illustrate the ε\varepsilon-rule process for ε=0.2\varepsilon=0.2 as an example. Then, in Figure 4 and Figure 5, we show the final patches for a few different values of ε\varepsilon.

Refer to caption
(a) α=(23)π\alpha=(2-\sqrt{3})\pi, β=γ=(31)π2\beta=\gamma=\frac{(\sqrt{3}-1)\pi}{2}
Refer to caption
(b) α=(21)π\alpha=(\sqrt{2}-1)\pi, β=γ=(22)π2\beta=\gamma=\frac{(2-\sqrt{2})\pi}{2}
Figure 3. Illustration of the ε\varepsilon-rule for ε=0.2\varepsilon=0.2 for optimal badly approximable angles.
Refer to caption
(a) ε=0.08\varepsilon=0.08
Refer to caption
(b) ε=0.04\varepsilon=0.04
Refer to caption
(c) ε=0.02\varepsilon=0.02
Figure 4. Final patches resulting from different ε\varepsilon-rules for optimal badly approximable angles α=(23)π\alpha=(2-\sqrt{3})\pi, β=γ=(31)π2\beta=\gamma=\frac{(\sqrt{3}-1)\pi}{2}.
Refer to caption
(a) ε=0.08\varepsilon=0.08
Refer to caption
(b) ε=0.04\varepsilon=0.04
Refer to caption
(c) ε=0.02\varepsilon=0.02
Figure 5. Final patches resulting from different ε\varepsilon-rules for optimal badly approximable angles α=(21)π\alpha=(\sqrt{2}-1)\pi, β=γ=(22)π2\beta=\gamma=\frac{(2-\sqrt{2})\pi}{2}.

As described in [19, Remark 4.11], one can produce a stationary tiling by applying an additional isometry after each ε\varepsilon-rule. For our subdivision rule shown in Figure 1, we can do this by introducing a rotation by the badly approximable angle γ-\gamma.

To make this more precise, choose the sequence εn=ε0n\varepsilon_{n}=\varepsilon_{0}^{n} where ε0=t2(1+t2)2\varepsilon_{0}=\frac{t^{2}}{(1+t^{2})^{2}} and t=sin(α)sin(β)t=\frac{\sin(\alpha)}{\sin(\beta)}. Then ε0\varepsilon_{0} is the square of the contraction factor of the similitude f3f_{3} in (4.12). This function maps the large scalene triangle T1T_{1} shown on the left in Figure 1 to the smaller scalene triangle in its center. For this value of ε0\varepsilon_{0}, the finite patch 𝒫ε0(T1){\mathcal{P}}_{\varepsilon_{0}}(T_{1}) contains a copy of eiγT1e^{i\gamma}T_{1}. With this choice of εn\varepsilon_{n}, the sequence einγ(𝒫εn(T1))e^{-in\gamma}({\mathcal{P}}_{\varepsilon_{n}}(T_{1})) will produce a stationary tiling. Figure 6 shows the resulting nested sequence of finite patches when α\alpha and β=γ\beta=\gamma are as in (4.1)\eqref{eq:optimal1-angles} and (4.2).

Refer to caption
(a) α=(23)π\alpha=(2-\sqrt{3})\pi, β=γ=(31)π2\beta=\gamma=\frac{(\sqrt{3}-1)\pi}{2}
Refer to caption
(b) α=(21)π\alpha=(\sqrt{2}-1)\pi, β=γ=(22)π2\beta=\gamma=\frac{(2-\sqrt{2})\pi}{2}
Figure 6. Illustration of the sequences producing stationary tilings for badly approximable angles. The stationary tiling is produced by choosing εn=ε0n\varepsilon_{n}=\varepsilon_{0}^{n} where ε0\varepsilon_{0} such that the area of the middle triangle is preserved, and applying an appropriate isometry after applying each εn\varepsilon_{n}-rule. Each stationary subpatch is highlighted in blue. In (B), an additional rotation by π4\frac{\pi}{4} is applied for ease of illustration.

Each finite patch in these nested sequences contains the previous finite patch, along with several new copies of the triangle rotated by badly approximable angles α\alpha and β=γ\beta=\gamma. Due to these irrational rotations, we expect the diffraction from the resulting stationary tilings to be rotationally invariant. Moreover, the discrepancy of each irrational rotation is small and optimal for our two choices of angles.

We conclude this section with a remark on convergence.

Remark 4.11.

The tilings produced by our method have infinite local complexity; because of this, we utilized the Chabauty–Fell topology to show the existence of a limit Delone set via a non-constructive process of subsequence selection. However, by the method described above, we can always produce a nested sequence of finite patches converging to a stationary tiling. In this case, we also have convergence in the local topology, i.e. the finite patches overlap exactly out to larger and larger radii up to small translations (see [2, Chapter 5] for a formal definition). This stronger notion of convergence is primarily used in the study of tilings with finite local complexity, but is still applicable stationary constructions.

5. Open Problems

In Theorem 1.6, we prove that there are exactly two solutions of the equality x+y+z=1x+y+z=1 in 2,1{\mathcal{B}}_{2,1} and that these solutions are in (2){\mathbb{Q}}(\sqrt{2}) and (3){\mathbb{Q}}(\sqrt{3}). In 2,2{\mathcal{B}}_{2,2}, we obtain at least three additional solutions of the equation x+y+z=1(xyz)x+y+z=1(x\leq y\leq z):

x=y=[3,3,1,2¯],z=[2,1,1,2¯];\displaystyle x=y=[3,3,\overline{1,2}]\,,\quad z=[2,1,\overline{1,2}]\,;
x=y=[3,1,1,2¯],z=[2,3,1,2¯];\displaystyle x=y=[3,1,\overline{1,2}]\,,\quad z=[2,3,\overline{1,2}]\,;
x=[3,1,1,2¯],y=[3,3,1,2¯],z=[2,2,2,2,1¯].\displaystyle x=[3,1,\overline{1,2}]\,,\quad y=[3,3,\overline{1,2}]\,,\quad z=[2,2,2,\overline{2,1}]\,.

However, we do not know whether or not the number of solutions is finite in 2,j(j2){\mathcal{B}}_{2,j}({\color[rgb]{1,0,1}j\geq 2}) and whether or not they are in a real quadratic field. In Theorem 1.8, we prove that there are infinitely many solutions of the equality x+y+z=1x+y+z=1 in 2{\mathcal{B}}_{2}^{*}, but we do not know how large the set of solutions is, or its Hausdorff dimension. We know that the number of solutions changes from finite to infinite as we go from 2,1{\mathcal{B}}_{2,1} to 2{\mathcal{B}}_{2}^{*}, but what happens in between?

The proof of Theorem 1.8 relied on the two key identities (3.2) and (3.1). In fact, many similar identities can be found. For example,

1[2,1,3,1x1][2,1,3,1y1][3,1,1,11xy]\displaystyle 1-[2,1,3,\tfrac{1}{x}-1]-[2,1,3,\tfrac{1}{y}-1]-[3,1,1,\tfrac{1}{1-x-y}] =4(xy)2(8x11)(8y11)(114x4y),\displaystyle=\frac{4(x-y)^{2}}{(8x-11)(8y-11)(11-4x-4y)}\,,
1[3,1,1,1x][3,1,1,1y][2,3,1,11xy1]\displaystyle 1-[3,1,1,\tfrac{1}{x}]-[3,1,1,\tfrac{1}{y}]-[2,3,1,\tfrac{1}{1-x-y}-1] =2(xy)2(4x+7)(4y+7)(2x+2y+7),\displaystyle=-\frac{2(x-y)^{2}}{(4x+7)(4y+7)(2x+2y+7)}\,,
1[3,3,1,1x2][3,3,1,1y2][2,1,1,1,1xy]\displaystyle 1-[3,3,1,\tfrac{1}{x}-2]-[3,3,1,\tfrac{1}{y}-2]-[2,1,1,1,1-x-y] =8(xy)2(16x13)(16y13)(138x8y).\displaystyle=\frac{8(x-y)^{2}}{(16x-13)(16y-13)(13-8x-8y)}\,.

From such identities whose right side is divisible by xyx-y, we can construct further explicit solutions of x+y+z=1x+y+z=1 in 2{\mathcal{B}}_{2}^{*} or 3{\mathcal{B}}_{3}. It may be an interesting problem to characterize the set of such identities. Such transformations on xx form a semi-group of integral Möbius transformations, but can we describe its generators? Are they finite? Moreover, our method produces many isosceles triangles, but we know very little about scalene triangles. Below, we point out a sporadic infinite family of solutions to x+y+z=1x+y+z=1 of this type:

x=[3,(2),1,1,2¯],y=[3,(2),3,1,2¯],z=[(2)4+2,1,2¯]=0,1,,x=[3,(2)^{\ell},1,\overline{1,2}]\,,\quad y=[3,(2)^{\ell},3,\overline{1,2}]\,,\quad z=[(2)^{4+2\ell},\overline{1,2}]\qquad\ell=0,1,\dots\,,

which is shown by induction using the two lucky equalities:

1[3,1x1][3,1y1][2,2,11xy]\displaystyle 1-[3,\tfrac{1}{x}-1]-[3,\tfrac{1}{y}-1]-[2,2,\tfrac{1}{1-x-y}] =2(x+y3)(2xy2x2y+1)(2x3)(2y3)(72x2y),\displaystyle=\frac{2(x+y-3)(2xy-2x-2y+1)}{(2x-3)(2y-3)(7-2x-2y)}\,,
2[3,1x1][3,1y1]2[3,1x1]2[3,1y1]+1\displaystyle 2[3,\tfrac{1}{x}-1][3,\tfrac{1}{y}-1]-2[3,\tfrac{1}{x}-1]-2[3,\tfrac{1}{y}-1]+1 =2xy2x2y+1(2x3)(2y3).\displaystyle=-\frac{2xy-2x-2y+1}{(2x-3)(2y-3)}\,.

Lastly, regarding the diffraction from the Delone sets obtained in Section 4, an interesting open problem is to determine how the continued fraction expansions of the badly approximable numbers xx, yy, zz are related to the autocorrelation measures of the associated Delone sets; see [2, Chapter 9] for an overview of the theory of diffraction from point sets.

Appendix A Proof of compactness of Wr,R(2)W_{r,R}({\mathbb{R}}^{2})

For completeness, here we give a proof that Wr,R(2)W_{r,R}({\mathbb{R}}^{2}) is compact in the Chabauty–Fell topology. Note that to obtain the desired compactness of Wr,R(2)W_{r,R}({\mathbb{R}}^{2}), it is necessary to use open balls for uniform discreteness and closed balls for relative denseness in the definition of an (r,R)(r,R)-Delone set.

Lemma A.1.

The set

𝒲r,R(2)={Y22:Yis an(r,R)-Delone set in2},{\mathcal{W}}_{r,R}({\mathbb{R}}^{2})=\{Y\in 2^{{\mathbb{R}}^{2}}\,:\,Y\ \text{is an}\ (r,R)\text{-Delone set in}\ {\mathbb{R}}^{2}\}\,,

is compact in the Chabauty–Fell topology.

Proof.

It follows from the early work of Fell [6] that the space 2X2^{X} is compact in the Chabauty–Fell topology for every topological space XX. Let X=2X={\mathbb{R}}^{2}. Since 𝒲r,R(X)2X{\mathcal{W}}_{r,R}(X)\subseteq 2^{X}, it suffices to show that 𝒲r,R(X){\mathcal{W}}_{r,R}(X) is closed. To this end, let {Λn}n1\{\Lambda_{n}\}_{n\geq 1} be a sequence in 𝒲r,R(X){\mathcal{W}}_{r,R}(X) converging to some Λ2X\Lambda\in 2^{X}. Our goal is to prove that Λ\Lambda is both rr-uniformly discrete and RR-relatively dense.

Proof of rr-uniform discreteness. Let xXx\in X be arbitrary. Suppose by contradiction that there are two points y,zΛB(x,r)y,z\in\Lambda\cap B(x,r) with yzy\neq z. Consider any

0<ε<min(1r+x,rxy,rxz,12yz).0<\varepsilon<\min(\textstyle{\frac{1}{r+\|x\|}},r-\|x-y\|,r-\|x-z\|,\textstyle{\frac{1}{2}}\|y-z\|)\,.

By convergence in the Chabauty–Fell topology, there exists an N1N\geq 1 such that

ΛB(0,1ε)Λn+B(0,ε)nN.\Lambda\cap B(0,\textstyle{\frac{1}{\varepsilon}})\subseteq\Lambda_{n}+B(0,\varepsilon)\quad\forall n\geq N\,.

Now, since ε<1r+x\varepsilon<\frac{1}{r+\|x\|}, we have that B(x,r)B(0,1ε)B(x,r)\subseteq B(0,\textstyle{\frac{1}{\varepsilon}}), so

y,zΛB(x,r)ΛB(0,1ε)Λn+B(0,ε)nN.y,z\in\Lambda\cap B(x,r)\subseteq\Lambda\cap B(0,\textstyle{\frac{1}{\varepsilon}})\subseteq\Lambda_{n}+B(0,\varepsilon)\quad\forall n\geq N\,.

In particular, there exist points yNy_{N} and zNz_{N} in ΛN\Lambda_{N} such that yyN<ε\|y-y_{N}\|<\varepsilon and zzN<ε\|z-z_{N}\|<\varepsilon. By our choice of ε\varepsilon, we have yz>2ε\|y-z\|>2\varepsilon. From this, we see that

yNzNyzyyNzzN>2εεε=0,\|y_{N}-z_{N}\|\geq\|y-z\|-\|y-y_{N}\|-\|z-z_{N}\|>2\varepsilon-\varepsilon-\varepsilon=0\,,

so yNzNy_{N}\neq z_{N}. Furthermore, we have rxy>εr-\|x-y\|>\varepsilon and rxz>εr-\|x-z\|>\varepsilon, so yNy_{N} and zNz_{N} are both in B(x,r)B(x,r). Indeed, we have

xyNxy+yyN<rε+ε=r,\|x-y_{N}\|\leq\|x-y\|+\|y-y_{N}\|<r-\varepsilon+\varepsilon=r\,,

and a similar inequality shows that xzN<r\|x-z_{N}\|<r. This contradicts rr-uniform discreteness of ΛN\Lambda_{N}. Therefore, ΛB(x,r)\Lambda\cap B(x,r) has at most one element for every x2x\in{\mathbb{R}}^{2}, i.e. Λ\Lambda is rr-uniformly discrete.

Proof of RR-relative denseness. Let xXx\in X be arbitrary. We aim to show that ΛB(x,R)¯\Lambda\cap\overline{B(x,R)}\neq\emptyset. By assumption, we have that Λn\Lambda_{n} is RR-relatively dense for every nn, so there exists a sequence of points yny_{n} in XX such that ynΛnB(x,R)¯y_{n}\in\Lambda_{n}\cap\overline{B(x,R)} for all nn. Since B(x,R)¯\overline{B(x,R)} is compact in XX (in the Euclidean topology), there exists a subsequence yniy_{n_{i}} of yny_{n} and some yB(x,R)¯y\in\overline{B(x,R)} such that yniy0\|y_{n_{i}}-y\|\rightarrow 0. Next, observe that for all nn\in{\mathbb{N}} with n>R+x+1n>R+\|x\|+1, we have B(x,R)¯B(0,n)\overline{B(x,R)}\subseteq B(0,n). From this and convergence in the Chabauty–Fell topology, there exists an N>R+x+1N>R+\|x\|+1 such that

ynΛnB(x,R)¯ΛnB(0,n)Λ+B(0,1n)nN.y_{n}\in\Lambda_{n}\cap\overline{B(x,R)}\subseteq\Lambda_{n}\cap B(0,n)\subseteq\Lambda+B(0,\textstyle{\frac{1}{n}})\quad\forall n\geq N\,.

Thus, there is a sequence znz_{n} in Λ\Lambda such that ynzn<1n\|y_{n}-z_{n}\|<\frac{1}{n} for all nNn\geq N. In particular, we have zniyz_{n_{i}}\rightarrow y. Now, since Λ\Lambda is a closed set in the Euclidean topology, we must have yΛy\in\Lambda. Moreover, yy is also in B(x,R)¯\overline{B(x,R)}, so we have shown that there is some yΛB(x,R)¯y\in\Lambda\cap\overline{B(x,R)}\neq\emptyset, as desired. This completes the proof.

Acknowledgements

S.A. is supported by JSPS grants 20K03528, 24K06662 and RIMS in Kyoto University. E.R.K. is supported by the Natural Sciences and Engineering Research Council of Canada (NSERC) via grant 2024-0485 and the Canadian Graduate Scholarship - Doctoral. Y-L.X. is supported by the China Scholarship Council, China (No. 202306770085). We would also like to thank Nicolae Strungaru for his insights on the construction of Delone sets, and Noel Murasko for his assistance in producing the graphics.

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