1 Introduction
In 1984, Schettmann discovered new solids with a clear diffraction pattern and 5-fold symmetry [Reference Shechtman, Blech, Gratias and Cahn30]. This discovery led to a paradigm shift in physics, as for more than 100 years, clear diffraction patterns have been thought to be the identifying signature of periodic crystals, and thus incompatible with 5-fold rotational symmetry. The newly discovered materials are now called quasicrystals.
The standard method for producing mathematical models for quasicrystals is via a cut and project scheme (or on short CPS). This method was introduced in the 1970s by Meyer [Reference Meyer22] in order to produce point sets with certain harmonic properties and was rediscovered by deBruijn [Reference de Bruijn8] when studying the construction of the Penrose tiling [Reference Penrose26] via the Ammann bars. Meyer’s pioneering work in the study of CPSs was popularized and expanded in the 1990s by Moody [Reference Moody and Moody23, Reference Moody25] and Lagarias [Reference Lagarias17, Reference Lagarias, Baake and Moody18]. The basic idea beyond CPSs is the following: to produce a model for a three-dimensional quasicrystal, we start with a lattice
${\mathcal L}$
in a higher dimensional space which sits at an irrational angle with respect to our space, cut a strip of the lattice which is within bounded distance (the “window”) of the three-dimensional space, and project the lattice points in this strip on our space. If the shape of the strip is not too bad, the point set produced via the CPS should still show some residue of long-range order from the lattice
${\mathcal L}$
(see, e.g., [Reference Hof and Patera10, Reference Hof11, Reference Schlottmann, Baake and Moody29, Reference Solomyak and Patera31]). In general, if the window is “bad,” the diffraction can have a continuous component but the pure point and (singular/absolutely) continuous components still show high coherence [Reference Strungaru33–Reference Strungaru36].
Recently, results about model sets have been extended to a larger class of such models called weak model sets of maximal density [Reference Baake, Huck and Strungaru4, Reference Keller13–Reference Keller and Richard15]. This class contains many models of number theoretic origin, such as square free integers, visible points of a lattice,
${\mathcal B}$
-free integers, and coprime families of lattices [Reference Baake and Huck3, Reference Baake, Moody and Pleasants6, Reference Dymek, Kasjan, Kułaga-Przymus and Lemańczyk9]. A key result in this settings is a theorem by Moody [Reference Moody, Axel, Dénoyer and Gazeau24] which states that for any CPS and any compact window, almost surely all positions of the window give maximal density weak model sets, and hence point sets with pure point diffraction. Similar results can be shown for open precompact windows [Reference Baake, Huck and Strungaru4], but it was not clear so far how to extend these results beyond topological windows. It is our goal to extend these results to precompact Borel windows in this article, by using some new developments into the theory of Besicovitch almost periodic measures [Reference Lenz, Spindeler and Strungaru20, Reference Lenz, Spindeler and Strungaru21], and the connection between pure point diffraction and dynamical spectra and mean, Besicovitch and Weyl almost periodicity.
In this article, given a CPS
$(G,H,{\mathcal L})$
, a precompact Borel window B, and a tempered van Hove sequence
${\mathcal A}$
, we prove the existence of a set
$\mathcal {MG}(B) \subseteq \mathbb T$
of full Haar measure such that, for all
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, the set
is Besicovitch almost periodic with respect to
${\mathcal A}$
and has autocorrelation
$\gamma $
and diffraction
$\widehat {\gamma }$
(with respect to
${\mathcal A}$
) given by
where
$c(B)$
denotes the covariogram of B (see below for definitions and notations). We further show that for all
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, the set
has well-defined Fourier–Bohr coefficients
$a_{\chi }^{{\mathcal A}}$
with respect to
${\mathcal A}$
, and

In particular, the consistent phase property (CPP) holds.
Furthermore, we show that there exists an ergodic measure
$\mathfrak { m}$
on the extended hull
such that, for all
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, the set
is generic for
$\mathfrak { m}$
. In particular,
$\mathfrak { m}$
has pure point spectrum, autocorrelation
$\gamma $
, and diffraction
$\widehat {\gamma }$
given by (1.1) and (1.2), respectively.
We should also note that recently, the same results have been established via dynamical systems in [Reference Keller, Richard and Strungaru16]. The approach we use below is via Besicovitch almost periodic measures and can be seen as a complement to [Reference Keller, Richard and Strungaru16].
2 Preliminaries
For the entire article, G denotes a second countable locally compact Abelian group (LCAG). We will denote by
$C_{\text{u}}(G)$
the space of uniformly continuous bounded functions on G, and by
$C_{\text{c}}(G)$
the subspace of compactly supported continuous functions. The Haar measure on G is denoted by
$\theta _G$
. For a Borel set
$B \subseteq G$
, we will often use the notation
$|B|:= \theta _G(B)$
.
We collect, in this section, some of the necessary background and standard notations needed to read this article. Since this article builds on [Reference Baake, Huck and Strungaru4] and uses many results from [Reference Lenz, Spindeler and Strungaru20, Reference Lenz, Spindeler and Strungaru21], for brevity, we refer the reader to those papers for most standard definitions and notations.
2.1 Cut and project schemes
We briefly review the definition of cut and project schemes and properties of weak model sets. For more details, we recommend [Reference Baake and Grimm1, Reference Baake and Grimm2, Reference Lenz and Richard19, Reference Moody and Moody23, Reference Moody, Axel, Dénoyer and Gazeau24, Reference Richard and Strungaru27, Reference Strungaru, Baake and Grimm35, Reference Strungaru36], just to name a few.
Definition 2.1 By a cut and project scheme (or simply CPS), we understand a triple
$(G,H, {\mathcal L})$
consisting of two LCAG
$G,H$
, and a lattice
${\mathcal L} \subseteq G \times H$
with the following properties:
-
• The restriction of the first projection $\pi _G|_{{\mathcal L}}$
to
${\mathcal L}$
is one-to-one. -
• $\pi _{H}({\mathcal L})$
is dense in H.
Given a CPS
$(G,H, {\mathcal L})$
, we denote by
$\mathbb T:=(G \times H) /{\mathcal L}$
and by
$L:= \pi _G({\mathcal L})$
. There exists a mapping, call the star mapping,
$\star : L \to H$
so that
${\mathcal L}= \{ (x,x^\star ) : x \in L \}$
. Next, for each
$W \subseteq H$
, we can define
We are interested in
, when W is a precompact Borel set. For such set
$W \subseteq H$
, we define its covariogram function
$c_W : H \to {\mathbb C}$
via
$c_W(t):= \theta _{H}(W \cap (t+W))$
.
More generally, for each
$h : H \to {\mathbb C}$
, we can define a formal sum
If h is compactly supported and bounded, then
$\omega _h$
is a measure. There are many other conditions on h which ensure that
$\omega _h$
is a measure; see, for example, [Reference Lenz and Richard19, Reference Richard and Strungaru27, Reference Strungaru36, Reference Strungaru37].
Note here that, for all
$s \in L$
, we have
We will often use these two formulas.
Given a CPS
$(G,H, {\mathcal L})$
, we can define
Then,
$(\widehat {G}, \widehat {H}, {\mathcal L}^0)$
is a CPS[Reference Moody and Moody23], called the CPS dual to
$(G, H, {\mathcal L})$
. This dual CPS plays the central role in the study of diffraction of model sets.
To avoid confusion, for each
$h : \widehat {H} \to {\mathbb C}$
, we will denote the comb given by h in the dual CPS
$(\widehat {G}, \widehat {H}, {\mathcal L}^0)$
by
$\omega ^\star _{h}$
, that is,
When dealing with functions, one can use Følner sequences to calculate averages (means). Below, we will often calculate the average (density) of point sets, and in this situation, Følner sets do not suffice. Indeed, the sequence
which is the interval
$[-n-\frac {1}{2}, n+\frac {1}{2}]$
with small holes around the integers, is a Følner sequence which cannot be used to average the Delone set
${\mathbb Z}$
, or weighted Dirac combs on
${\mathbb Z}$
. Similarly, for each Delone subset
$\Lambda \subseteq {\mathbb R}$
, it is easy to construct a Følner sequence which has an empty intersection with
$\Lambda $
.
As it was observed by Schlottmann [Reference Schlottmann, Baake and Moody29], to avoid this issue when dealing with point sets or measures, one needs to work instead with van Hove sequences (see [Reference Lenz, Spindeler and Strungaru20, Definition 1.6] for definition and properties). Any van Hove sequence is a Følner sequence, and any
$\sigma $
-compact LCAG G admits a (tempered) van Hove sequence.
Given a uniformly discrete set
$\Lambda \subseteq G$
and a van Hove sequence
${\mathcal A}=\{A_k\}$
, we define
If the following limit exists, or equivalently if
$\underline {\mathrm {dens}}_{{\mathcal A}}(\Lambda )=\overline {\mathrm {dens}}_{{\mathcal A}}(\Lambda )$
, we define
Let us next recall the following result of [Reference Huck and Richard12].
Theorem 2.1 [Reference Huck and Richard12]
Let
$(G,H, {\mathcal L})$
be a CPS and
$W \subseteq H$
be a precompact. Then, for all van Hove sequences
${\mathcal A}$
, we have
We will use the following definitions.
Definition 2.2 Let
$(G,H, {\mathcal L})$
be a CPS and let
$W \subseteq H$
be a precompact.
-
(a) If W is compact, we call
a weak model set. -
(b) If W is open, we call
a open model set. -
(c) We say that
has maximal density with respect to
${\mathcal A}$
if $$\begin{align*}\mathrm{dens}_{{\mathcal A}}( \curlywedge (W)) = \mathrm{dens}({\mathcal L}) \theta_H(\overline{W}). \end{align*}$$
-
(d) We say that
has minimal density with respect to
${\mathcal A}$
if $$\begin{align*}\mathrm{dens}_{{\mathcal A}}( \curlywedge (W)) = \mathrm{dens}({\mathcal L}) \theta_H(W^\circ). \end{align*}$$
Remark 2.2
-
(a) If
has maximal density with respect to
${\mathcal A}$
, then
is a maximal density weak model set. Such models have been studied in [Reference Baake, Huck and Strungaru4, Reference Keller13–Reference Keller and Richard15]. -
(b) If
has minimal density with respect to
${\mathcal A}$
, then
is a minimal density open model set. We derive the theory of such models in the next section, from the theory of maximal density weak model sets.
Let us complete this section by recalling the following result from [Reference Moody25].
Theorem 2.3 [Reference Moody25, Theorem 1]
Let
$(G,H, {\mathcal L})$
be a CPS, let
$W \subseteq H$
be a measurable precompact set, and let
${\mathcal A}$
be a tempered van Hove sequence in G. Then, for almost all
$(s,t)+{\mathcal L} \in (G \times H)/ {\mathcal L} =: \mathbb T$
, we haveFootnote
1
2.2 Dynamical systems
Next, we review few basic facts about dynamical systems of translation bounded measures. Let us start by recalling the following result of [Reference Spindeler and Strungaru32] (compare [Reference Baake and Lenz5]).
Lemma 2.4 [Reference Spindeler and Strungaru32]
Let
$\mathbb X \subseteq {\mathcal M}^\infty (G)$
be any G invariant vaguely closed set. Then,
$\mathbb X$
is vaguely compact if and only if there exists some C and an open precompact set
$\emptyset \neq U \subseteq G$
such that
Moreover, in this case, the vague topology on
$\mathbb X$
is metrizable.
Next, let us review the following definition, which is inspired by the general Birkhoff ergodic theorem for continuous group actions [Reference Chatard7, Reference Tempelman38].
Definition 2.3 Let
$(X,G,\mathfrak { m})$
be an ergodic dynamical system and let
${\mathcal A}$
be a van Hove sequence. An element
$x \in X$
is called generic for
$\mathfrak { m}$
if
holds for all
$f \in C(X)$
.
We will need the following simple characterizations of generic elements. This has been used implicitly in [Reference Baake and Lenz5, Reference Lenz, Spindeler and Strungaru20, Reference Lenz, Spindeler and Strungaru21] just to name a few. Since the result is well known and trivial to prove, we skip the proof.
Proposition 2.5 Let
$(X, G, \mathfrak { m})$
be an ergodic dynamical system. Then,
$x \in X$
is generic for
$\mathfrak { m}$
if and only if the set of
$f \in C(X)$
for which
is dense in
$C(X)$
.
By combining this result with Stone–Weierstrass theorem, we immediately get the following proposition.
Proposition 2.6 Let
$\mathbb X \subseteq {\mathcal M}_{C,U}$
be vaguely compact and G-invariant, and let
$\mathfrak { m}$
be an ergodic measure on
$\mathbb X$
. If all measures in
$\mathbb X$
are real valued, then a measure
$\mu \in \mathbb X$
is generic for
$\mathfrak { m}$
if and only if, for all
$n \in \mathbb N$
and
$\varphi _1,\ldots , \varphi _n \in C_{\text {c}}(G)$
, we have
2.3 The hull and extended hull
Recall that, for a precompact open set
$\emptyset \neq U \neq \subseteq G$
, we denote by
$\mathcal {D}_U$
the set of U-uniformly discrete subsets of G. The mapping
$\Lambda \to \delta _{\Lambda }$
induces an embedding of
$\mathcal {D}_U$
into
${\mathcal M}_{1, U}$
with compact range. We can then equip
$\mathcal {D}_U$
with the local rubber topology
$\tau _{lr}$
, which is the pullback through this mapping of the vague topology.
Now, let
$(G, H, {\mathcal L})$
be a cut and project scheme and
$B \subseteq H$
be any precompact set. Then, there exists some precompact open set
$\emptyset \neq U \neq \subseteq G$
such that, for all
$(s,t) \in G \times H$
, we have
.
Definition 2.4 The hull
of
and extended hull
${\mathcal M}_B^G$
of B are defined as

where the closure is taken in the local rubber topology.
Remark 2.7 As observed by Schlottmann [Reference Schlottmann, Baake and Moody29], we get a natural G-mapping
Moody’s uniform distribution result, Theorem 2.3, implies that almost surely almost all positions
$(s,t)+{\mathcal L} \in G \times H / {\mathcal L}$
give us point sets whose distributional average in G matches the corresponding integrals over the window. Since we are interested in those elements, and since the original position may not be one of those generic positions, one needs to work with the extended hull
${\mathcal M}_B^G$
and not just the classical hull
.
For regular model sets, we have
, but this is in general not true. Indeed, consider the CPS
$({\mathbb R}, H, {\mathcal L})$
and the window W of the visible points of the lattice [Reference Baake, Huck and Strungaru4]. Then, there exists positions
$t \in H$
such that
$(t+W) \cap L^\star =\emptyset $
. Pick one such position t and set
$B=t+W$
. Then,
while the extended hull
${\mathcal M}_B^G$
contains the visible points of the lattice.
From a dynamical point of view, the above mapping can be seen as a (generally) discontinuous observation introduced by the window on the compact group
$\mathbb T$
. We will show below that there exists a natural measure (the Mirsky measure) which describes the distribution generated by the observation, and that almost all
$(s,t)+{\mathcal L} \in \mathbb T$
define observations
which are generic for this measure.
We complete this section by proving the following simple lemma.
Lemma 2.8 Let
$(G,H,{\mathcal L})$
be a CPS and
$h \in C_{\textsf {c}}(H)$
and let
$\mathfrak { m}$
denote the unique ergodic measure on
$\mathbb X(\omega _h)$
. Then,
-
(a) For all $t \in H$
, we have
$\omega _{\tau _th} \in \mathbb X(\omega _g)$
. -
(b) For all $f \in C(\mathbb X(\omega _h))$
and all
$(s,t) \in G \times H$
, we have $$\begin{align*}\mathfrak{ m}(f)= \lim_k \frac{1}{|A_k|} \int_{A_k} f( \tau_{s+x} \omega_{\tau_t h}) \mathrm{d} x. \end{align*}$$
Proof “(a)” Since
$L^\star $
is dense in H, we can find a precompact neighborhood
$t \in V$
and a net
$t_{\alpha }$
with
$t_\alpha \in V$
which converges in H to t. Then, using the uniform continuity of h, we get that
Next, all these functions are supported in the compact set
$\overline {V}+\mathrm {supp}(h)$
. Therefore, all the measures
$\omega _{ \tau _{t_\alpha }h}, \omega _{ \tau _{t}h}$
are supported inside the uniformly discrete set
. Moreover, (2.5) implies that for all
, we have
This combined with the equi uniform discreteness of their support implies that
$\omega _{ \tau _{t_\alpha }h}$
converges vaguely to
$\omega _{ \tau _{t}h}$
.
Finally, since
$t_\alpha \in L^\star $
, there exists some
$s_\alpha \in L$
such that
$t_\alpha = s_\alpha ^\star $
. Then, by (2.2), we have
The claim follows.
“(b)” follows immediately from (a) and the unique ergodic theorem.
2.4 Besicovitch almost periodicity
Consider a Følner sequence
${\mathcal A}$
on G. On the space of a locally bounded measurable function, we can then define a semi-norm, called the Besicovitch p-seminorm for functions
With this in mind, let us recall the following definition.
Definition 2.5 A function
$f \in L^1_{loc}(G)$
is called Besicovitch
$1$
-almost periodic if for each
$\varepsilon>0$
there exists a Bohr almost periodic function g such that
A translation bounded measure
$\mu $
is called Besicovitch almost periodic if
$\mu *\varphi $
is a Besicovitch
$1$
-almost periodic function for all
$\varphi \in C_{\textsf {c}}(G)$
.
The space of Besicovitch almost periodic measures is denoted by
$\mathcal {AP}\text {-}{Bes}_{{\mathcal A}}(G)$
.
In this article, we will be interested in point sets
$\Lambda $
for which
$\delta _{\Lambda } \in \mathcal {AP}\text {-}{Bes}_{{\mathcal A}}(G)$
. Because of this, we introduce the following notation:
Below, we will make use of the following two results.
Theorem 2.9 [Reference Lenz, Spindeler and Strungaru20, Theorem 4.39]
Let
$\mu \in {\mathcal M}^\infty (G)$
and let
${\mathcal A}$
be a van Hove sequence. Then,
$\mu \in \mathcal {AP}\text {-}{Bes}_{{\mathcal A}}(G)$
if and only if the following three conditions hold:
-
• The autocorrelation $\gamma $
of
$\mu $
exists with respect to
${\mathcal A}$
and
$\widehat {\gamma }$
is pure point. -
• For each $\chi \in \widehat {G}$
, the Fourier–Bohr coefficient $$\begin{align*}a_\chi^{\mathcal A}(\mu):= \lim_k \frac{1}{|A_k|}\int_{A_k} \overline{\chi(t)} \mathrm{d} \mu(t) \end{align*}$$
exists.
-
• For each $\chi \in \widehat {G}$
, we have $$\begin{align*}\widehat{\gamma}(\{\chi\}) = \left| a_\chi^{\mathcal A}(\mu)\right|^2. \end{align*}$$
Theorem 2.10 [Reference Lenz, Spindeler and Strungaru20, Theorem 7.28]
Let
$\mu \in \mathcal {AP}\text {-}{Bes}_{{\mathcal A}}(G)$
and let
${\mathcal A}$
be a van Hove sequence. Then, there exists an ergodic measure
$\mathfrak { m}$
on
$\mathbb X(\mu )$
with pure point spectrum such that
$\mu $
is generic for
$\mathfrak { m}$
with respect to
${\mathcal A}$
.
For a measure
$\mu \in {\mathcal M}^\infty $
, we will denote by
For all
$\varphi \in C_{\text {c}}(G)$
and
$\mu \in {\mathcal M}^\infty (G)$
, we have [Reference Lenz, Spindeler and Strungaru20, Lemma 2.13]
3 Minimal density open model sets
In this section, we review the theory of minimal density open model sets, deducing all important results from the corresponding theory of maximal density weak model sets from [Reference Baake, Huck and Strungaru4]. We also derive new results.
Lemma 3.1 Let
$(G, H, {\mathcal L})$
be a CPS and let
$U \subseteq H$
be a precompact open set and K a regular window such that
$U \subseteq K$
. Then,
-
(a)
. -
(b)
has maximal density with respect to
${\mathcal A}$
if and only if
has minimal density with respect to
${\mathcal A}$
.
Proof “(a)” is obvious.
“(b)” First note that since
$U \subseteq K$
, we have
Now, by (a), we have
Therefore,

Next, since K is regular model set, we have
The claim follows.
As consequence, we get (compare [Reference Baake, Huck and Strungaru4]).
Theorem 3.2 Let
${\mathcal A}$
be a van Hove sequence,
$(G,H, {\mathcal L})$
be a CPS, and let
be a minimal density open model set with respect to
${\mathcal A}$
. Then,
-
(a)
. -
(b) The autocorrelation $\gamma $
of
exists and satisfies $$\begin{align*}\gamma=\mathrm{dens}({\mathcal L}) \omega_{c_U} = \mathrm{dens}( {\mathcal L}) \sum_{(x,x^\star) \in {\mathcal L}} \theta_H(U \cap (x^\star +U)) \delta_x. \end{align*}$$
-
(c) The diffraction $\widehat {\gamma }$
is given by $$\begin{align*}\widehat{\gamma}= \mathrm{dens}({\mathcal L})^2 \sum_{(\chi,\chi^\star) \in {\mathcal L}^0} \left| \int_{U} \chi^\star(t) \mathrm{d} t \right|^2 \delta_\chi =(\mathrm{dens}({\mathcal L}))^2 \omega^\star_{|\check{1_U}|^2}\,. \end{align*}$$
-
(d) The Fourier–Bohr coefficients

exist and satisfy

-
(e)
satisfies the CPP 
-
(f) There exists a G-invariant ergodic measure $\mathfrak { m}$
on
such that
is generic for
$\mathfrak { m}$
. -
(g) $(\mathbb X, G, \mathfrak { m})$
has a pure point dynamical spectrum. -
(h) $\gamma $
is the autocorrelation of
$(\mathbb X, G, \mathfrak { m})$
.
Proof “(a)” Pick some regular set K such that
$U \subseteq K$
. Then,
By [Reference Lenz, Spindeler and Strungaru20, Corollary 5.35],
is Weyl almost periodic and hence Besicovitch almost periodic with respect to
${\mathcal A}$
. Moreover,
has maximal density and hence
[Reference Lenz, Spindeler and Strungaru20, Proposition 4.45]. Thus,
.
“(b),(c), (d)” follow from [Reference Baake, Huck and Strungaru4, Theorem 9].
“(e)” follows from [Reference Baake, Huck and Strungaru4, Theorem 9] or [Reference Lenz, Spindeler and Strungaru20, Theorem 4.39].
“(f),(g)” follow from Theorem 2.10.
“(h)” follows from [Reference Lenz, Spindeler and Strungaru20, Theorem 7.20].
4 Model sets with Borel windows
For the entire section,
$(G, H, {\mathcal L})$
is a fixed CPS and
$B \subseteq H$
is a fixed Borel precompact set. Since B is precompact,
$\theta _H(B) < \infty $
. We introduce now some important players for the construction of the ergodic measure and of its generic elements.
4.1 Construction of
$\boldsymbol{U_n, K_n,}$
and
$\boldsymbol{g_n}$
For each n, by [Reference Rudin28, Theorem 2.14(c) and (d)], there exists some compact set
$K_n$
and open precompact set
$U_n \subseteq U$
such that
We fix one such choice of
$K_n$
and
$U_n$
for each n and, by eventually replacing
$K_n$
by
$K_1 \cup K_2 \cup \cdots \cup K_n$
and
$U_n$
by
$U_1 \cap U_2 \cap \cdots \cap U_n$
, we can assume without loss of generality that
Next, for each n, fix some
$g_n \in C_{\textsf {c}}(G)$
such that
$1_{K_n} \leq g_n \leq 1_{U_n}$
. The sets
$K_n, U_n$
and the functions
$g_n$
are fixed for the remaining of the section.
We can now introduce the following definition.
Definition 4.1 We denote by
and we will refer to this as the set of fb-generic points.
Remark 4.1 While the definition of
$\mathcal {MG}(B)$
seems to depend on the choice of
$g_n$
, Lemma 4.8 shows that it does not. Lemma 4.8 will also explain the choice of name.
Lemma 4.2 Let
$(s,t)+{\mathcal L} \in \mathbb T$
. Then,
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
if and only if, for all
$\varphi \in C_{\textsf {c}}(G)$
, we have
Proof
$\Longrightarrow $
follows from (2.6).
$\Longleftarrow $
We know that
which is uniformly discrete. Let
$V \subseteq G$
be any open set such that
is V-uniformly discrete. Then,
is
$v+V$
-uniformly discrete for all
$v \in G$
.
Let
$C:= \{ \varphi \in C_{\textsf {c}}(G) : \exists v \in G \text { s.t. } \mathrm {supp}(\varphi )\subseteq v+V \}$
. Strungaru [Reference Strungaru, Baake and Grimm35, Lemma 5.8.3] implies that for all
$\varphi \in C$
, we have
This immediately implies that
for all
$\varphi \in C$
. As
$\text {Span}(C) =C_{\textsf {c}}(G)$
, the claim follows.
4.2 The main result
For each n, define

and let
By Theorem 2.3,
$X_n, Y_n \subseteq \mathbb T$
contain subsets of full measure in
$\mathbb T$
. In particular, since we assume the Haar measure to be complete,
$X_n$
and
$Y_n$
have full measure in
$\mathbb T$
. It follows that
$\theta _{\mathbb T}({\mathcal T}) =1$
. Note here that
$(s,t) +{\mathcal L} \in {\mathcal T}$
if and only if for all n, we have
We can now prove the following result (compare [Reference Keller, Richard and Strungaru16, Theorem 4.6]).
Theorem 4.3 Let
$(G,H, {\mathcal L})$
be a CPS, let
$B \subseteq H$
be a Borel precompact set, and let
${\mathcal T} \subseteq \mathbb T$
be as in (4.1). Then,
-
(a) We have ${\mathcal T} \subseteq \mathcal {MG}(B)$
. In particular,
$\mathcal {MG}(B)$
has full measure in
$\mathbb T$
. -
(b) For all $(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, we have
. -
(c) For each $(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, we have 
-
(d) For each $(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, the autocorrelation
$\gamma $
of
exists, is independent of the choice of
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, and satisfies $$\begin{align*}\gamma=\mathrm{dens}({\mathcal L}) \omega_{c(B)} = \mathrm{dens}( {\mathcal L}) \sum_{(x,x^\star) \in {\mathcal L}} \theta_H(B \cap (x^\star +B)) \delta_x. \end{align*}$$
-
(e) The diffraction $\widehat {\gamma }$
is given by $$\begin{align*}\widehat{\gamma}= \mathrm{dens}({\mathcal L})^2 \sum_{(\chi,\chi^\star) \in {\mathcal L}^0} \left| \int_{B} \chi^\star(t) \mathrm{d} t \right|^2 \delta_\chi=(\mathrm{dens}({\mathcal L}))^2 \omega^\star_{|\check{1_B}|^2}. \end{align*}$$
-
(f) For each $(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, the Fourier–Bohr coefficients 
exist and satisfy

-
(g) For all $(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, the set
satisfies the CPP 
Proof “(a)” Let
$(s,t)+{\mathcal L} \in {\mathcal T}$
. We have

which together with (4.2) and (4.3) gives
Thus,
which proves (a).
“(b)” Let
$(s,t) +{\mathcal L} \in \mathcal {MG}(B)$
. Then, (2.6) gives that for all
$\varphi \in C_{\textsf {c}}(G)$
, we have
Since
$ \tau _{-s}\omega _{\tau _{t}g_n} \in \mathcal {AP}\text {-}{Strong} (G)$
, (b) follows.
“(c,d,e,f,g)” Let
$(s,t) +{\mathcal L} \in \mathcal {MG}(B)$
. Since
, for each character
$\chi $
, the Fourier–Bohr coefficient
exists by [Reference Lenz, Spindeler and Strungaru20, Proposition 4.32].
Moreover, for all
$\varphi \in C_{\textsf {c}}(G)$
, we have

with the second inequality following from (4.4) the inequality
$\left |a_\chi ^{\mathcal A}(f)\right | \leq \|f\|_{{\textsf {B}},1,{\mathcal A}}$
. This shows that
Now, when
$\chi =0$
is the trivial character, (4.5) yields (c).
Next, since
, the autocorrelation
$\gamma $
of
exists with respect to
${\mathcal A}$
, is strongly almost periodic, and satisfies [Reference Lenz, Spindeler and Strungaru20, Theorem 4.39].
which is (g).
Moreover, since
(f) follows. Moreover, combining (f) with the fact that
$\gamma $
is strongly almost periodic and satisfies the CPP, we get (e).
Finally, the measure
$\eta := \mathrm {dens}({\mathcal L}) \omega _{c(B)}$
is positive definite and hence Fourier transformable. Moreover,
with the second equality following from (e). This yields (d).
By combining Theorem 4.3 with Theorem 2.10, we get the following corollary.
Corollary 4.4 Let
$(G,H, {\mathcal L})$
be a CPS, let
$B \subseteq H$
be a Borel precompact set, and let
${\mathcal T} \subseteq \mathbb T$
be as in (4.1). Then, for each
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, there exists an ergodic measure
$\mathfrak { m}_{(s,t)+{\mathcal L}}$
on
such that
is generic for
$\mathfrak { m}_{(x,t)+{\mathcal L}}$
.
In the next section, we are going to prove that
$\mathfrak { m}_{(s,t)+{\mathcal L}}$
does not depend on the choice of
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
.
4.3 The Mirsky measure
We can now introduce the Mirsky measure associated with the window B. Since
$\omega _{g_n}$
are strongly almost periodic, the hull
$\mathbb X(\omega _{g_n} )$
is uniquely ergodic. Let
$\mathfrak { m}_n$
be the unique ergodic measure on
$\mathbb X(\omega _{g_n} )$
. We will show that for all
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, the sequence
$\mathfrak { m}_n$
converges vaguely to
$\mathfrak { m}_{(s,t)+{\mathcal L}}$
.
By construction, all measures
$\omega _n$
are supported inside the model set
. It follows immediately that there exists some open precompact set U and some
$C>0$
such that all the hulls
$\mathbb X(\omega _n)$
and
${\mathcal M}_B^G$
are subsets of
${\mathcal M}_{C,U}$
. This set is G-invariant and vaguely compact [Reference Baake and Lenz5]. Let
$\mathbb Y$
denote the set of real valued measures in
${\mathcal M}_{C,K}$
. Then,
$\mathbb Y$
is G invariant, vaguely compact, and contains
$\mathbb X(g_n)$
and
${\mathcal M}_B^G$
. Also, we can consider the measures
$\mathfrak { m}_n$
and
$\mathfrak { m}_{(s,t)+{\mathcal L}}$
as measures on
$\mathbb Y$
.
As usual, for
$\phi \in C_{\textsf {c}}(G)$
, we define
$F_{\phi } : \mathbb Y \to {\mathbb C}$
via
Since
$\mathbb Y$
only consists of real valued measures, we have
$\overline {F_{\phi }}= F_{\overline {\phi }}$
.
Let us first prove the following preliminary lemma.
Lemma 4.5 Let
$\phi _1, \ldots , \phi _j \in C_{\textsf {c}}(G)$
. Then, for all
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
, we have

Proof The limit

exists by the Besicovitch almost periodicity of
. A short computation shows

where
Therefore, the definition of
$\mathcal {MG}(B)$
and (2.6) give

Finally, by Lemma 2.8 and the unique ergodicity of
$m_n$
, we have
which proves the claim.
We can now prove that all
$m_{(s,t)+{\mathcal L}}$
are the same.
Proposition 4.6 For each
$(s,t) +{\mathcal L} \in \mathcal {MG}(B)$
, the measures
$\mathfrak { m}_n$
converge vaguely on
$\mathbb Y$
to
$\mathfrak { m}_{(s,t)+{\mathcal L}}$
. In particular,
$\mathfrak { m}_{(s,t)+{\mathcal L}}$
is the same for all
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
.
Proof Fix an arbitrary
$(s,t) +{\mathcal L} \in \mathcal {MG}(B)$
Consider the algebra
$\mathbb A$
generated by
$\{ F_{\phi }: \phi \in C_{\textsf {c}}(G) \} \cup \{ 1_{\mathbb Y} \}$
, which is dense in
$C(\mathbb Y)$
.
Since
$ (s,t)+ {\mathcal L} \in \mathcal {MG}(B)$
, the measure
is generic for
$\mathfrak { m}_{(s,t)+{\mathcal L}}$
and hence, for all
$\varphi _1, \ldots , \varphi _j \in C_{\textsf {c}}(G)$
, we have

This together with Lemma 4.5 gives that for all
$\varphi _1, \ldots , \varphi _j \in C_{\textsf {c}}(G)$
, we have
Now, since
$\mathfrak { m}_{(s,t)+{\mathcal L}}(1_{\mathbb Y})=1=\mathfrak { m}_n(1_{\mathbb Y})$
, it follows immediately that
Since G is second countable and
$\mathbb Y$
is metrizable and compact, the set
$\text {Prob}(\mathbb Y)$
of probability measures on
$\mathbb Y$
is vaguely compact and metrizable. Therefore, to show that
$m_n$
converges vaguely to
$\mathfrak { m}_{(s,t)+{\mathcal L}}$
, it suffices to show that
$\mathfrak { m}_{(s,t)+{\mathcal L}}$
is the unique vague cluster point of
$\mathfrak { m}_n$
. Let
$\mathfrak { m}$
be any vague cluster point of
$\mathfrak { m}_n$
. Then, (4.7) yields
Therefore, the denseness of
$\mathbb A$
gives
$\mathfrak { m}_{(s,t)+{\mathcal L}}=\mathfrak { m}$
, completing the proof.
This leads to the next definition, compare [Reference Keller, Richard and Strungaru16].
Definition 4.2 We define the Mirsky measure
$Q_{B}^G$
of B as
By combining Theorem 4.3, Proposition 4.6, and [Reference Lenz, Spindeler and Strungaru20, Reference Lenz, Spindeler and Strungaru21], we get the following proposition.
Proposition 4.7 Let
$(G,H, {\mathcal L})$
be a CPS and
$B \subseteq H$
be a Borel precompact set. Then,
-
(a) For all $(s,t) +{\mathcal L} \in \mathcal {MG}(B)$
, the set
is generic for
$Q_B^G$
. -
(b) $({\mathcal M}_B^G, G, Q_{B}^G)$
has a pure point dynamical spectrum. Moreover, the dynamical spectrum is generated by the set
$\{ \chi : \widehat {\gamma }(\{\chi \}) \neq 0 \}$
of Bragg peak positions. -
(c) $\gamma $
is the autocorrelation of
$({\mathcal M}_B^G, G, Q_{B}^G)$
. -
(d) $Q_{B}^G( {\mathcal M}_B^G \cap \mathcal {AP}\text {-}{Bes}_{{\mathcal A},ps}(G))=1$
. -
(e) For each $\chi $
with
$\widehat {\gamma }(\{ \chi \}) \neq 0$
, the function $$\begin{align*}{\mathcal M}_B^G \cap \mathcal{AP}\text{-}{Bes}_{{\mathcal A},ps}(G) \ni \omega \to a_{\chi}^{{\mathcal A}} ( \omega) \end{align*}$$
is a measurable eigenfunction for ${\mathcal M}_B^G$
.
We complete the section by characterizing
$\mathcal {MG}(B)$
in terms of genericity with respect to the Mirsky measure and Fourier–Bohr coefficients.
Lemma 4.8 Let
$(s,t) +{\mathcal L} \in \mathbb T$
. Then,
$(s,t) +{\mathcal L} \in \mathcal {MG}(B)$
if and only if
and

In particular,
$\mathcal {MG}(B)$
does not depend on the choice of
$U_n, K_n$
, and
$g_n$
.
Proof
$\Longrightarrow $
follows from Theorem 4.3.
$\Longleftarrow $
Let
$0 \in V \subseteq G$
be open such that
is V-uniformly discrete. Pick some
$\varphi \in C_{\textsf {c}}(G)$
such that
$\varphi \geq 0, \int \varphi =1$
, and
$\mathrm {supp}(\varphi ) \subseteq V$
.
Since
is Besicovitch almost periodic, we have by the Parseval identity

with the last equality following from the Poisson summation formula [Reference Richard and Strungaru27].
Note here that
$\left ( (\varphi ^\dagger )*\widetilde {(\varphi ^\dagger )} \otimes (1_B -g_m)*\widetilde {(1_B-g_m)} \right )$
are supported inside a fixed compact set, and hence
$ \delta _{{\mathcal L}} \left ( (\varphi ^\dagger )*\widetilde {(\varphi ^\dagger )} \otimes (1_B -g_m)*\widetilde {(1_B-g_m)} \right )$
is a finite sum. Since
$\left ( (\varphi ^\dagger )*\widetilde {(\varphi ^\dagger )} \otimes (1_B -g_m)*\widetilde {(1_B-g_m)} \right )$
converge point wisely to
$0$
, we get
and hence by [Reference Lenz, Spindeler and Strungaru20, Lemma 2.7], we have
Finally, the choice of
$\varphi $
and [Reference Strungaru, Baake and Grimm35, Lemma 5.8.3] give the claim.
Remark 4.9 (Independence of the Mirsky measure of various choices)
Here, we explain why the Mirsky measure does not depend on the various choices we made.
-
(a) The Mirsky measure $Q_{B}^G$
does not depend on the choice of
$U_n, K_n$
, and
$g_n$
. Indeed, for a fixed tempered van Hove sequence
${\mathcal A}$
, by Lemma 4.8, the set
$\mathcal {MG}(B)$
does not depend on the choice of
$U_n, K_n$
, and
$g_n$
. Since for each
$(s,t)+{\mathcal L} \in \mathcal {MG}(B)$
the measure
is generic for the Mirsky measure, and since any element in the dynamical system can be generic for at most one ergodic measure with respect to
${\mathcal A}$
, the Mirsky measure is the same for all choices of
$U_n, K_n$
, and
$g_n$
. -
(b) The Mirsky measure $Q_{B}^G$
does not depend on the choice of the van Hove sequence
${\mathcal A}$
but the set
$\mathcal {MG}(B)$
usually does depend on this choice. In particular, the elements
which are generic with respect to
$Q_{B}^G$
depend on the choice of
${\mathcal A}$
.The independence of $Q_{B}^G$
of
${\mathcal A}$
is immediate. Indeed, given some precompact Borel set
$B \subseteq H$
, we can construct the sets
$U_n, K_n$
, and the function
$g_n$
, and these constructions are independent of the choice of
${\mathcal A}$
. Now, the dynamical system
$\mathbb X(\omega _{g_n})$
is uniquely ergodic, and hence the choice of the unique ergodic measure
$\mathfrak { m}_n$
on
$\mathbb X(\omega _{g_n})$
does not depend on the choice of
${\mathcal A}$
. As
$Q_{B}^G$
is the vague limit of
$\mathfrak { m}_n$
, it is also independent on the choice of
${\mathcal A}$
.On the other hand, since $\mathcal {MG}(B)$
uniquely determine the generic Besicovitch almost periodic elements in
$({\mathcal M}_B^G, G, Q_{B}^G)$
, and since
${\mathcal M}_B^G$
is usually not uniquely ergodic, it is easy to construct examples where different choices of
${\mathcal A}$
lead to different generic Besicovitch almost periodic elements. -
(c) In [Reference Keller, Richard and Strungaru16], the Mirsky measure $Q_B^G$
is introduced as the push forward of the Haar measure
$\theta _{\mathbb T}$
through the measurable function 
Lemma 4.8 and [Reference Keller, Richard and Strungaru16, Theorem 4.6] imply that the two constructions produce the same measure.
Points (a) and (b) above then follow alternately from the observation that the construction in [Reference Keller, Richard and Strungaru16] does not depend on these choices.
5 Some examples with Borel windows
Consider a CPS
$(G,H,{\mathcal L})$
and a precompact Borel window B. Let
. Theorem 4.3 gives the inclusion
Moreover, when B is topological (meaning open or closed), the above inclusion is equality [Reference Baake, Huck and Strungaru4, Reference Keller and Richard14].
We give below a class of examples with Borel window for which this inclusion is strict. First, let us prove the following simple lemma.
Lemma 5.1 Let
$({\mathbb R}^d, {\mathbb R}^m, {\mathcal L})$
be any fully Euclidean CPS with one to one star mapping. Let
$W \subset {\mathbb R}^m$
be any regular model set and
be any subset. Then, for each
$0 <a <\infty $
, there exists some precompact Borel set
$B_a$
such that
Here,
$\lambda $
denotes the Lebesgue measure on
${\mathbb R}^m$
.
Proof Define
Then,
$\pi _{{\mathbb R}^m}({\mathcal L})$
is countable. In particular,
$W_0$
is at most countable and hence it is Borel and satisfies
$\lambda (W_0)=0$
. Moreover, since
$\star $
is one to one we have
.
Next, pick some t such that
$t+ [0, \sqrt [m]{a}]^m \cap W = \emptyset $
. Define
Then,
$W_1$
is Borel,
$\lambda (W_1) = a$
and
. The set
$B_a=W_0 \cup W_1$
satisfies the desired conditions.
Now, we can easily construct counterexamples. Pick, for example, the Fibonacci CPS
$({\mathbb R}, {\mathbb R}, {\mathcal L})$
and window, and let
be the Fibonacci model set. Pick a subset
which is not pure point diffractive with respect to
$A_n =[-n, n]$
, for example, a generic point set for the Bernoullisation of Fibonacci. Set
$a =\mathrm {dens}_{{\mathcal A}}(\Gamma )$
and pick the window
$B_a$
from Lemma 5.1. Then, by the construction of
$B_a$
, for this Borel window, we have
On the other hand, since every element in
$\mathbb Y$
has pure point diffraction, we have
$\Gamma \notin \mathbb Y$
.
Acknowledgments
The author is grateful to Michael Baake, Gerhard Keller, Daniel Lenz, Christoph Richard, and Timo Spindeler for many insightful discussions about weak model sets and almost periodic measures, which were very helpful for this article. The author would also like to thank the anonymous reviewer for some comments which improved the quality of this manuscript.



