Constructive Approximation

, Volume 48, Issue 1, pp 163–182

# The Projective Ensemble and Distribution of Points in Odd-Dimensional Spheres

• Carlos Beltrán
• Ujué Etayo
Article

## Abstract

We consider a determinantal point process on the complex projective space that reduces to the so-called spherical ensemble for complex dimension 1 under identification of the 2-sphere with the Riemann sphere. Through this determinantal point process, we propose a new point processs in odd-dimensional spheres that produces fairly well-distributed points, in the sense that the expected value of the Riesz 2-energy for these collections of points is smaller than all previously known bounds.

## Keywords

Determinantal point processes Minimal Riesz energy Minimal Green energy

## Mathematics Subject Classification

Primary 31C12 Secondary 31C20 52A40

## 1 Introduction

Given $$s\in (0,\infty )$$, the Riesz s-energy of a set of points $$\omega _{n} = \{ x_{1}, \ldots ,x_{n} \}$$ on a subset $$X\subseteq \mathbb {R}^{m}$$ is
\begin{aligned} \mathscr {E}_{s}(\omega _{n}) = \displaystyle \sum _{i \ne j} \frac{1}{\Vert x_{i} - x_{j} \Vert ^{s}}. \end{aligned}
This energy has a physical interpretation for some particular values of s; i.e., for $$s=1$$, the Riesz energy is the Coulomb potential, and for $$s=d-2$$ ($$d\ge 3$$), it is the Newtonian potential. In the special case $$s=0$$, the energy is defined by
\begin{aligned} \mathscr {E}_{0}(\omega _{n})=\left. \frac{d}{ds} \right| _{s=0}\mathscr {E}_{s}(\omega _n) = \sum _{i \ne j} \log \Vert x_{i} - x_{j} \Vert ^{-1} \end{aligned}
and is related to the transfinite diameter and the capacity of the set by classical potential theory, see for example [11].
The minimal value of this energy and its asymptotic behavior have been extensively studied, most remarkably in the case when $$X=\mathbb {S}^{d}\subseteq \mathbb {R}^{d+1}$$ is the d-dimensional unit sphere. In [7, 15], it was proved that for $$d > 2$$ and $$0<s<d$$, there exist constants $$c>C> 0$$ (depending only on d and s) such that
\begin{aligned} -cn^{1 + \frac{s}{d}} \le \min _{\omega _n}\left( \mathscr {E}_{s}(\omega _{n})\right) - V_{s}(\mathbb {S}^{d})n^{2} \le -Cn^{1 + \frac{s}{d}}, \end{aligned}
(1)
where $$V_{s}(\mathbb {S}^{d})$$ is the continuous s-energy for the normalized Lebesgue measure,
\begin{aligned} V_{s}(\mathbb {S}^{d}) = \frac{1}{Vol(\mathbb {S}^{d})^{2}} \displaystyle \int _{p,q \in \mathbb {S}^{d}} \frac{1}{\Vert p-q\Vert ^{s}}\mathrm{d}p\mathrm{d}q = 2^{d-s-1} \frac{\Gamma \left( \frac{d+1}{2} \right) \Gamma \left( \frac{d-s}{2} \right) }{\sqrt{\pi } \Gamma \left( d- \frac{s}{2} \right) }. \end{aligned}
Finding accurate bounds for the constants in (1) is an important open problem and has been addressed by several authors, see [5, 10, 17, 18] for some very precise conjectures and [8] or [6] for surveys. One can state the problem as follows:

### Problem 1.1

For $$s\in (0,d)$$, let $$C_{s,d,n}$$ be defined by
\begin{aligned} 0<C_{s,d,n}=\frac{ V_{s}(\mathbb {S}^{d})n^{2} -\min _{\omega _n}\left( \mathscr {E}_{s}(\omega _{n})\right) }{n^{1+\frac{s}{d}}}. \end{aligned}
Find asymptotic values for $$C_{s,d,n}$$ as $$n\rightarrow \infty$$. In particular, prove if the limit exists.

A sometimes successful strategy for the upper bound in the constant $$C_{s,d,n}$$ is to take collections of random points in $$\mathbb {S}^{d}$$ and then compute the expected value of the energy (which is of course greater than or equal to the minimum possible value). Simply taking n points with the uniform distribution in $$\mathbb {S}^{d}$$ already gives the correct term $$V_{s}(\mathbb {S}^{d})n^{2}$$, and other distributions with nice separation properties have proved successful in bounding the constant $$C_{s,d,n}$$.

We are thus interested in computationally feasible random procedures to generate points in sets that exhibit local repulsion. One natural choice is using determinantal point processes that have these two properties (see [13] for theoretical properties and [19] for an implementation). A brief summary of the fundamental properties of determinantal point processes is given in Sect. 2.

In a recent paper [1], a determinantal point process named the spherical ensemble is used to produce low-energy random configurations on $$\mathbb {S}^{2}$$. This process was previously studied by Krishnapur [14], who proved a remarkable fact: the spherical ensemble is equivalent to taking eigenvalues of $$A^{-1}B$$ (where AB have Gaussian entries) and sending them to the sphere through the stereographic projection.

In [2] a different determinantal point process rooted on the use of spherical harmonics is described, producing low-energy random configurations in $$\mathbb {S}^{d}$$ for some infinite sequence of values of n. In particular, it is proved in that paper that
\begin{aligned} \limsup _{n\rightarrow \infty } C_{s,d,n}\ge 2^{s-s/d}V_s(\mathbb {S}^{d}) \frac{ d\,\Gamma \left( 1+\frac{d}{2} \right) \Gamma \left( \frac{1+s}{2} \right) \Gamma \left( d-\frac{s}{2}\right) }{ \sqrt{\pi } \Gamma \left( 1+\frac{s}{2} \right) \Gamma \left( 1+\frac{s+d}{2} \right) \left( d!\right) ^{1-\frac{s}{d}}},\quad 0<s<d.\nonumber \\ \end{aligned}
(2)
If $$d-1<s<d$$, $$\limsup$$ can be changed to $$\liminf$$ in (2) (see [2, Cor. 2]). The bound in (2) is the best known to the date for general d (although more precise bounds exist for particular values of d, including $$d=1,2$$, see [5, 9]). In particular, for $$s=2$$ and odd dimensions, the formula in (2) reads
\begin{aligned} \limsup _{n\rightarrow \infty } C_{2,2d+1,n}\ge \frac{2^{1-\frac{2}{2d+1}}\left( {(2d+1)!}\right) ^\frac{2}{2d+1}}{(2d-1)(2d+3)}{\mathop {\rightarrow }\limits ^{d\rightarrow \infty }}\frac{2}{e^2}. \end{aligned}
(3)
The determinantal point process in [2] is called the harmonic ensemble, and it is shown to be the optimal one (at least for $$s=2$$) among a certain class of determinantal point processes obtained from subspaces of functions with real values defined in $$\mathbb {S}^{d}$$.

However, the bound in [2] for the case $$d=2$$ is worse than that of [1], which is not surprising since the spherical ensemble uses complex functions and is thus of a different nature.

An alternative natural interpretation of Krishnapur’s result is to consider eigenvalues $$(\alpha ,\beta )\in {\mathbb {P}}(\mathbb {C}^2)$$ of the generalized eigenvalue problem $$\det (\beta A-\alpha B)=0$$ and to identify $${\mathbb {P}}(\mathbb {C}^2)$$ with the Riemann sphere. A homotety then generates the points in the unit sphere $$\mathbb {S}^{2}$$. This remark suggests that the spherical ensemble can be seen as a natural point process in the complex projective space, and a search for an extension to higher dimensions is in order. In this paper, we use an extension of this process to $$\mathbb {P}(\mathbb {C}^{d+1})$$ for any $$d\ge 2$$. This process is indeed a particular case of a more general construction by Robert Berman [4]. We will propose the name projective ensemble.

In order to show the separation properties of the projective ensemble, we will define a (probably nondeterminantal) point process in odd-dimensional spheres, which will allow us to compare our results to those of [2]. This point process is as follows: first, choose a number r of points in $$\mathbb {P}(\mathbb {C}^{d+1})$$ coming from the projective ensemble. Then, consider k equally spaced unit norm affine representatives of each of the projective points. We allow these points to be rotated by a randomly chosen phase. As a result, we get rk points in the odd-dimensional sphere $$\mathbb {S}(\mathbb {C}^{d+1})\equiv \mathbb {S}^{2d+1}$$.

We study the expected 2-energy of such a point process, getting the bound in Theorem 1.2 below:

### Theorem 1.2

With the notation above,
\begin{aligned} \begin{aligned}&\limsup _{n\rightarrow \infty } C_{2,2d+1,n} \ge \frac{3^{1 - \frac{2}{2d+1}} (2d-1)^{1 - \frac{2}{2d+1}} (2d+1) \Gamma \left( d- \frac{1}{2} \right) ^{2 - \frac{2}{2d+1}}}{2^{4 - \frac{2}{2d+1}} (d!)^{2 - \frac{4}{2d+1}}}{\mathop {\rightarrow }\limits ^{d\rightarrow \infty }}\frac{3}{4e}. \end{aligned} \end{aligned}
(4)
The bound in Theorem 1.2 is larger than that of (3), which shows that random configurations of points coming from this point process are better distributed (in the sense that they have lower 2-energy on the average) than those coming from the harmonic ensemble. See Fig. 1 for a graphical comparison of both bounds.
Since the point process we have defined in $$\mathbb {S}^{2d+1}$$ starts by choosing points in $$\mathbb {P}(\mathbb {C}^{d+1})$$ coming from the projective ensemble, Theorem 1.2 gives us arguments to think that the projective ensemble produces quite well distributed points in $$\mathbb {P}(\mathbb {C}^{d+1})$$ (for $$d=1$$, this property is quantitatively described in [1]). There are several ways to measure how well distributed a collection of points is in $$\mathbb {P}(\mathbb {C}^{d+1})$$. For example, one can study the natural analogues of Riesz’s energy as we do in Theorem 3.3 below. A very natural measure is given by the value of Green’s energy of [3]: let $$G:\mathbb {P}(\mathbb {C}^{d+1})\times \mathbb {P}(\mathbb {C}^{d+1})\rightarrow [0,\infty ]$$ be the Green function for $$\mathbb {P}(\mathbb {C}^{d+1})$$; that is, $$G(x,\cdot )$$ is zero-mean for all x, G is symmetric and $$\Delta _yG(x,y)=\delta _x(y)-vol(\mathbb {P}(\mathbb {C}^{d+1}))^{-1}$$, with $$\delta _x$$ the Dirac’s delta function, in the distributional sense. The Green energy of a collection of r points $$\omega _r=(x_1,\ldots ,x_r)\in \mathbb {P}(\mathbb {C}^{d+1})^r$$ is defined as
\begin{aligned} \mathscr {E}_{G}^{\mathbb {P}}(\omega _r)=\sum _{i\ne j}G(x_i,x_j). \end{aligned}
Minimizers of Green’s energy are asymptotically well-distributed in the sense that they asymptotically approach the uniform distribution on any compact Riemannian manifold, see [3, Main Theorem]. Our second main result will follow from the computation of the expected value of Green’s energy for the projective ensemble.

### Theorem 1.3

Let $$d\ge 2$$. Then
\begin{aligned} \liminf _{r\rightarrow \infty }\frac{\min _{\omega _r}\left( \mathscr {E}_{G}^{\mathbb {P}}(\omega _{r})\right) }{r^{2 - \frac{1}{d}}}\le -\frac{ (d!)^{1 - \frac{1}{d}}}{4\pi ^{d} (d-1)}. \end{aligned}
(5)

If r points are chosen at random independently and uniformly on $$\mathbb {P}(\mathbb {C}^{d+1})$$, the expected value of their Green energy is exactly equal to 0, while Theorem 1.3 shows that for points coming from the projective ensemble, one can expect quite negative values of the energy. In other words, points coming from the projective ensemble, are better distributed than uniform random points. Theorem 1.3 also gives a criterion to decide how well-distributed a collection of projective points is: compute their Green’s energy and compare to that of (5).

## 2 Determinantal Point Processes

### 2.1 Basic Notions

In this section we follow [13].

### Definition 2.1

Let $$\Lambda$$ be a locally compact, Polish topological space with a Radon measure $$\mu$$. A simple point process $$\mathfrak {X}$$ of n points in $$\Lambda$$ is a random variable taking values in the space of n point subsets of $$\Lambda$$.

There are some subtle issues in the general definition of point processes, see [13, Section 1.2]. For our purposes, we will only use simple point processes with a fixed, finite number of points.

For some point processes, there exist joint intensities satisfying the following definition:

### Definition 2.2

Let $$\Lambda ,\mathfrak {X}$$ be as in Definition 2.1. The joint intensities are functions (if any exist) $$\rho _{k}:\Lambda ^k\rightarrow [0,\infty )$$, $$k\ge 1$$, such that for any family of mutually disjoint subsets $$D_1,\ldots ,D_k$$ of $$\Lambda$$, we have
\begin{aligned} \mathrm{E}_{x \sim \mathfrak {X}}\left[ \left( \prod _{i=1}^k \sharp (x\cap D_i)\right) \right] =\int _{\prod D_i}\rho _k(x_1,\ldots ,x_k)\,\mathrm{d}\mu (x_1,\ldots ,x_k). \end{aligned}
Here, $$\mathrm {E}$$ denotes expectation, and by $$x\sim \mathfrak {X}$$, we mean that x is a subset of $$\Lambda$$ with n elements, obtained from the point process $$\mathfrak {X}$$:
From [13, Formula (1.2.2)], for any measurable function $$\phi : \Lambda ^{k} \longrightarrow [0, \infty )$$, the following equality holds:
\begin{aligned}&\mathrm{E}_{x \sim \mathfrak {X}}\left[ \sum _{i_{1} \ldots i_{k}\text { distinct}} \phi (x_{i_{1}},\ldots , x_{i_{k}})\right] \nonumber \\&\quad =\int _{y_{1},\ldots ,y_{k} \in \Lambda } \phi (y_{1},\ldots ,y_{k}) \rho _{k}(y_{1},\ldots ,y_{k})\,\mathrm{d}\mu (y_1,\ldots ,y_k). \end{aligned}
(6)
Sometimes these intensity joint functions can be written as $$\rho _{k}(x_{1},\ldots ,x_{k}) = det(K(x_{i}, x_{j})_{i,j = 1,\ldots ,k})$$ for some measurable function $$K:\Lambda \times \Lambda \rightarrow \mathbb {C}$$. In this case, we say that $$\mathfrak {X}$$ is a determinantal point process. A particularly amenable collection of such processes is obtained from n-dimensional subspaces of the Hilbert space $$\mathrm {L}^2(\Lambda ,\mathbb {C})$$ (i.e., the set of square-integrable complex functions in $$\Lambda$$). Recall that the reproducing kernel of H is the unique continuous, skew-symmetric, positive-definite function $$K_H:\Lambda \times \Lambda \rightarrow \mathbb {C}$$ such that
\begin{aligned} f(x)=\langle f,K_H(\cdot ,x)\rangle =\int _{y\in \Lambda }f(y)K_H(x,y)\,\mathrm{d}y,\quad x\in \Lambda ,f\in H. \end{aligned}
Given any orthonormal basis $$\varphi _{1},\ldots ,\varphi _{n}$$ of H, we have
\begin{aligned} K_H(x,y)=\sum _{i=1}^n\varphi _i(x)\overline{\varphi _i(y)}. \end{aligned}
Such a kernel $$K_H$$ is usually called a projection kernel of trace n.

### Proposition 2.3

Let $$\Lambda$$ be as in Definition 2.1, and let $$H \subset \mathrm{L}^{2}(\Lambda ,\mathbb {C})$$ have dimension n. Then there exists a point process $$\mathfrak {X}_H$$ in $$\Lambda$$ of n points with associated joint intensity functions
\begin{aligned} \rho _{k}(x_{1},\ldots ,x_{k}) = det(K_H(x_{i}, x_{j})_{i,j = 1,\ldots ,k}). \end{aligned}
In particular, for any measurable function $$f:\Lambda \times \Lambda \longrightarrow [0,\infty )$$, we have
\begin{aligned}&\mathrm{E}_{x \sim \mathfrak {X}_H}\left[ \displaystyle \sum _{i \ne j} f(x_{i}, x_{j})\right] \\&\quad = \int _{p,q \in \Lambda } \left( K_H(p,p)K_H(q,q) - |K_H(p,q)|^{2} \right) f(p,q)\,\mathrm{d}\mu (p,q). \end{aligned}
We will call $$\mathfrak {X}_H$$ a projection determinantal point process with kernel $$K_H$$.

### Proof

This proposition is a direct consequence of the Macchi–Soshnikov theorem, see [16, 20] or [13, Theorem 4.5.5]. $$\square$$

### Remark 2.4

We note that in the hypotheses of Proposition 2.3, from (6) with $$\phi \equiv 1$$, we also have
\begin{aligned} n=\mathrm{E}_{x\sim \mathfrak {X}_H}\left[ n\right] = \int _{p\in \Lambda } K_H(p,p)\,\mathrm{d}\mu (p). \end{aligned}
In particular, if $$K_H(p,p)$$ is constant, then we must have $$K_H(p,p)=n/Vol(\Lambda )$$.

### 2.2 Transformation Under Diffeomorphisms

We now describe the push-forward of a projection determinantal point process. We are most interested in the case when the spaces are Riemannian manifolds (which are locally compact, Polish and measurable spaces).

### Proposition 2.5

Let $$\mathrm {M}_{1}$$ and $$\mathrm {M}_{2}$$ be two Riemannian manifolds, and let $$\phi : M_{1} \longrightarrow \mathrm {M}_{2}$$ be a $$\varvec{\mathscr {C}^{1}}$$ diffeomorphism. Let $$H \subset \mathrm {L}^{2}(\mathrm {M}_{1},\mathbb {C})$$ be an n-dimensional subspace. Then, the set
\begin{aligned} H_{*} =&\left\{ f: \mathrm {M}_{2} \longrightarrow \mathbb {C}: \sqrt{|\mathrm{Jac}(\phi )(\cdot )|}( f \circ \phi )(\cdot ) \in H \right\} \\ =&\left\{ g \circ \phi ^{-1}(\cdot )\sqrt{|\mathrm{Jac}(\phi ^{-1})(\cdot )|}: g \in H \right\} \end{aligned}
is an n-dimensional subspace of $$\mathrm {L}^2(\mathrm {M}_2,\mathbb {C})$$. Its associated determinantal point process $$\mathfrak {X}_{H_*}$$ has kernel
\begin{aligned} \begin{aligned} K_{H_*}(a,b)&= \frac{K_H(\phi ^{-1}(a), \phi ^{-1}(b))}{\sqrt{|\mathrm{Jac}(\phi )(\phi ^{-1}(a)) \mathrm{Jac}(\phi )(\phi ^{-1}(b))|}} \\&= K_H(\phi ^{-1}(a), \phi ^{-1}(b))\sqrt{|\mathrm{Jac}(\phi ^{-1})(a) \mathrm{Jac}(\phi ^{-1})(b)|}. \end{aligned} \end{aligned}
(We are denoting by $$\mathrm {Jac}$$ the Jacobian determinant).

This proposition is a direct consequence of the change of variables formula; see Sect. 5.1 for a short proof.

## 3 The Projective Ensemble

Consider the standard Fubini–Study metric in the complex projective space of complex dimension d, denoted by $$\mathbb {P}(\mathbb {C}^{d+1})$$. The distance between two points $$p,q\in \mathbb {P}(\mathbb {C}^{d+1})$$ is given by:
\begin{aligned} \sin d_{\mathbb {P}(\mathbb {C}^{d+1})}(p,q) = \sqrt{1 - \frac{| \left\langle p,q \right\rangle |^{2}}{|| q ||^{2} || p ||^{2}}} = \sqrt{1 - \left| \left\langle \frac{p}{||p||},\frac{q}{||q||}\right\rangle \right| ^{2}}. \end{aligned}

### Definition 3.1

Let $$L \ge 0$$, and consider the set of the following functions defined in $$\mathbb {C}^{d}$$:
\begin{aligned} I_{d,L} = \left\{ \sqrt{C_{\alpha _{1},\ldots ,\alpha _{d}}^{L}} \frac{z_{1}^{\alpha _{1}}\ldots z_{d}^{\alpha _{d}}}{(1+\Vert z\Vert ^{2})^{\frac{d+L+1}{2}}} \right\} _{\alpha _{1}+\ldots +\alpha _{d} \le L}, \end{aligned}
(7)
where $$\alpha _{1},\ldots ,\alpha _{d}$$ are non-negative integers and
\begin{aligned} C_{\alpha _{1},\ldots ,\alpha _{d}}^{L} = \frac{1}{{\pi }^{d}} \frac{(d+L)!}{\alpha _{1}!\ldots \alpha _{d}! (L-(\alpha _{1}+\ldots +\alpha _{d}))!}. \end{aligned}
Let $$\mathscr {H}_{d,L}=Span(I_{d,L})\subset \mathrm{L}^{2}(\mathbb {C}^{d},\mathbb {C})$$, which is a subspace of complex dimension $$r = {d+L \atopwithdelims ()d}$$. The collection $$I_{d,L}$$ given in (7) is an orthonormal basis of $$\mathscr {H}_{d,L}$$ (for the usual Lebesgue measure in $$\mathbb {C}^{d}$$), and the reproducing kernel $$K: \mathbb {C}^{d} \times \mathbb {C}^{d} \longrightarrow \mathbb {C}$$ is given by:
\begin{aligned} K(z,w) = \frac{r d!}{{\pi }^{d}} \frac{(1 + \left\langle z,w \right\rangle )^{L}}{(1+\Vert z\Vert ^{2})^{\frac{d+L+1}{2}} (1+\Vert w\Vert ^{2})^{\frac{d+L+1}{2}}}. \end{aligned}
From Proposition 2.3, there is an associated determinantal point process of r points in $$\mathbb {C}^d$$ that we denote by $$\mathfrak {X}^{(r,d)}$$.

### Lemma 3.2

Let $$L\ge 0$$, $$d\ge 1$$, and let r be of the form $$r={d+L \atopwithdelims ()d}$$. Then the pushforward $$\mathfrak {X}_*^{(r,d)}$$ of $$\mathfrak {X}^{(r,d)}$$ under the mapping
\begin{aligned} \begin{matrix} \psi _d:&{}\mathbb {C}^d&{}\rightarrow &{}\mathbb {P}(\mathbb {C}^{d+1}),\\ &{}z&{}\mapsto &{}(1,z) \end{matrix} \end{aligned}
is a determinantal point process in $$\mathbb {P}(\mathbb {C}^{d+1})$$ whose associated kernel satisfies
\begin{aligned} \left| K_*^{(r,d)}(p,q) \right| = \frac{r d!}{\pi ^{d}} \left| \left\langle \frac{p}{||p||}, \frac{q}{||q||} \right\rangle \right| ^L. \end{aligned}
We call this process the projective ensemble.

See Sect. 5.2 for a proof of Lemma 3.2. As pointed out above, a more general construction containing the projective ensemble has recently been described in [4].

The spherical ensemble described in [1, 14] is just the case $$d=1$$ of the projective ensemble identifying $$\mathbb {P}(\mathbb {C}^{2})$$ with the Riemann sphere and translating the process to the unit sphere.

The next result computes the expected value of a Riesz-like energy for the projective ensemble.

### Theorem 3.3

Let $$L\ge 1$$. For $$r=\left( {\begin{array}{c}d+L\\ d\end{array}}\right)$$ and $$\omega _{r}=(x_1,\ldots ,x_r)\in \mathbb {P}(\mathbb {C}^{d+1})^r$$, let
\begin{aligned} \mathscr {E}_{s}^{\mathbb {P}}(\omega _{r}) = \sum _{i \ne j} \frac{1}{\sin \left( d_{\mathbb {P}(\mathbb {C}^{d+1})} (x_{i}, x_{j}) \right) ^{s}}. \end{aligned}
Then, for $$0< s < 2d$$,
\begin{aligned} \begin{aligned} \mathrm{E}_{\mathfrak {X}_{*}^{(r,d)}}\left[ \mathscr {E}_{s}^{\mathbb {P}}(\omega _{r}) \right]&= \frac{d}{d - \frac{s}{2}}r^{2} - r^{2}dB \left( d - \frac{s}{2}, L + 1 \right) \\&= \frac{d}{d - \frac{s}{2}}r^{2}-r^{1+\frac{s}{2d}}\frac{d \Gamma \left( d - \frac{s}{2}\right) }{(d!)^{1-\frac{s}{2d}}}+o\left( r^{1+\frac{s}{2d}}\right) . \end{aligned} \end{aligned}
Note that $$d/(d-s/2)$$ is precisely the continuous s-energy for the uniform measure in $$\mathbb {P}(\mathbb {C}^{d+1})$$.

### Corollary 3.4

Let $$L\ge 1$$. For $$r=\left( {\begin{array}{c}d+L\\ d\end{array}}\right)$$ and $$\omega _{r}=(x_1,\ldots ,x_r)\in \mathbb {P}(\mathbb {C}^{d+1})^r$$, let
\begin{aligned} \mathscr {E}_{0}^{\mathbb {P}}(\omega _{r}) = \sum _{i \ne j} \log \frac{1}{\sin \left( d_{\mathbb {P}(\mathbb {C}^{d+1})} (x_{i}, x_{j}) \right) }. \end{aligned}
Then
\begin{aligned} \begin{aligned} \mathrm{E}_{\mathfrak {X}_{*}^{(r,d)}}\left[ \mathscr {E}_{0}^{\mathbb {P}}(\omega _{r}) \right]&= \frac{r^2}{2d}+\frac{r^2d}{2}B(d,L+1)\sum _{j=0}^L\frac{1}{d+j}\\&= \frac{r^2}{2d}+\frac{r\log r}{2d}+o\left( r\log r\right) . \end{aligned} \end{aligned}

Theorem 3.3 and Corollary  3.4 are proved in Sects. 5.3 and 5.4.

## 4 A New Point Process in Odd-Dimensional Spheres

We now describe a point process of n points, for certain values of n, in $$\mathbb {S}^{2d+1}$$ in the following manner.

### Definition 4.1

Given integers $$d,\,k,\,L\ge 0$$, let $$r=\left( {\begin{array}{c}d+L\\ d\end{array}}\right)$$ and $$n=k\,r$$. We define the following point process of n points in $$\mathbb {S}^{2d+1}$$. First, let
\begin{aligned} x_1,\ldots ,x_r\in \mathbb {P}(\mathbb {C}^{d+1})\end{aligned}
be chosen from the projective ensemble $$\mathfrak {X}_*^{(r,d)}$$. Choose, for each $$x_i$$, one affine representative (which we denote by the same letter). Then, let $$\theta _1,\ldots ,\theta _r\in [0,2\pi )$$ be chosen uniformly and independently, and define
\begin{aligned} y_{i}^{j} = e^{\mathbf {i}\left( \theta _{i} + \frac{2\pi j}{k} \right) } x_{i},\quad 1\le i\le r,\;0\le j\le k-1. \end{aligned}
(8)
We denote this point process by $$\mathfrak {X}_{\mathbb {S}^{2d+1}}^{(k,L)}$$.

Note that the way to generate a collection of n points coming from $$\mathfrak {X}_{\mathbb {S}^{2d+1}}^{(k,L)}$$ amounts to taking r points from the projective ensemble and taking, for each of these points, k affine unit norm representatives, uniformly spaced in the great circle corresponding to each point, with a random phase.

The following statement shows that the expected 2-energy of points generated from the point process of Definition 4.1 can be computed with high precision. It will be proved in Sect. 5.5.

### Proposition 4.2

\begin{aligned}&\mathrm{E}_{\mathfrak {X}_{\mathbb {S}^{2d+1}}^{(k,L)}}\left[ \mathscr {E}_{2}(y_{1}^{0},\ldots ,y_{1}^{k-1},\ldots ,y_{r}^{0},\ldots ,y_{r}^{k-1})\right] \nonumber \\&\quad =\frac{d}{2d-1} (kr)^{2}+\frac{rk^{3}}{12}-\frac{d\Gamma \left( d-\frac{1}{2}\right) }{2(d!)^{1-\frac{1}{2d}}} k^2r^{1+\frac{1}{2d}}+o\left( k^2r^{1+\frac{1}{2d}}\right) . \end{aligned}
(9)

Following the same ideas, one can also compute the expected s-energy for n points coming from the point process $$\mathfrak {X}_{\mathbb {S}^{2d+1}}^{(k,L)}$$ for other even integer values $$s \in 2\mathbb {N}$$, and a bound can be found for other values of $$s>0$$. The computations, though, are quite involved.

Proposition 4.2 describes how different choices of L (i.e., of r) and k produce different values of the expected 2-energy of the associated $$n=rk$$ points. An optimization argument is in order: for given n, which is the optimal choice of r and k? Since we know from (1) that the second-order term in the asymptotics is $$\sim n^{1+2/(2d+1)}=(rk)^{1+2/(2d+1)}$$, it is easy to conclude that the optimal values of r and k satisfy
\begin{aligned} k\sim r^{\frac{1}{2d}}. \end{aligned}
The following corollary follows inmediately from Proposition 4.2.

### Corollary 4.3

If we choose a positive integer $$k=A r^{\frac{1}{2d}}$$ for some $$A\in \mathbb {R}$$ (thus making $$n=kr$$ also an integer), then
\begin{aligned}&\mathrm{E}_{\mathfrak {X}_{\mathbb {S}^{2d+1}}^{(k,L)}}\left[ \mathscr {E}_{2}(y_{1}^{0},\ldots ,y_{1}^{k-1},\ldots ,y_{r}^{0},\ldots ,y_{r}^{k-1})\right] \nonumber \\&\quad = \frac{d}{2d-1} n^{2} + \left( \frac{A^{2 - \frac{2}{2d+1}} }{12} - \frac{d \Gamma \left( d - \frac{1}{2} \right) A^{1 - \frac{2}{2d+1}} }{2 \left( d!\right) ^{1 - \frac{1}{2d}} } \right) n^{1+\frac{2}{2d+1}} + o\left( n^{1+\frac{2}{2d+1}}\right) . \end{aligned}
(10)

The proof of our first main theorem will follow easily from Corollary 4.3.

## 5 Proof of the Main Results

### 5.1 Proof of Proposition 2.5

We first prove that $$H_*\subseteq \mathrm {L}^2(\mathrm {M}_2,\mathbb {C})$$. Indeed, for $$f\in H_*$$, we have
\begin{aligned} \int _{y\in \mathrm {M}_2}|f|^2\,\mathrm{d}y=\int _{y\in \mathrm {M}_2}|g\circ \phi ^{-1}(y)|^2|\mathrm {Jac}(\phi ^{-1})(y)|\,\mathrm{d}y \end{aligned}
for some $$g\in H$$. We thus have $$H_*\subseteq \mathrm {L}^2(\mathrm {M}_2,\mathbb {C})$$. Now, since $$H_*$$ is in one-to-one linear correspondence with H, the dimension of $$H_*$$ is also n. Now, by the change of variables formula, this last equals the squared $$\text {L}^2$$ norm of g, which is finite since $$H\subseteq \mathrm {L}^2(\mathrm {M}_1,\mathbb {C})$$.
We now prove the formula for $$K_{H*}$$. Let $$\varphi _1,\ldots ,\varphi _n$$ be an orthonormal basis of H. Then $$\varphi _{i,*}=\varphi _i \circ \phi ^{-1}(\cdot )\sqrt{|\mathrm{Jac}(\phi ^{-1})(\cdot )|}$$, $$1\le i\le n$$, are elements in $$H_*$$, and using the change of variables formula, we have
\begin{aligned} \int _{y\in \mathrm {M}_2} \varphi _{i,*}(y)\overline{\varphi _{j,*}(y)}\,\mathrm{d}y=&\int _{y\in \mathrm {M}_2} \varphi _i \circ \phi ^{-1}(y)\,\overline{\varphi _j \circ \phi ^{-1}(y)}\,|\mathrm{Jac}(\phi ^{-1})(y)|\,\mathrm{d}y\nonumber \\ =&\int _{x\in \mathrm {M}_1}\varphi _i(x)\overline{\varphi _j(y)}\,\mathrm{d}x=\delta _{ij}, \end{aligned}
where we use the Kronecker delta notation. Hence, $$\{\varphi _{i,*}\}$$ form an orthonormal basis, and
\begin{aligned} K_{H_*}(a,b)=&\sum _{i=1}^n\varphi _{i,*}(a)\overline{\varphi _{i,*}(b)}\\ =&\sum _{i=1}^n\varphi _i \circ \phi ^{-1}(a)\overline{\varphi _i \circ \phi ^{-1}(b)}\sqrt{|\mathrm{Jac}(\phi ^{-1})(a)\,\mathrm{Jac}(\phi ^{-1})(b)|}\\ =&K_H(\phi ^{-1}(a), \phi ^{-1}(b))\sqrt{|\mathrm{Jac}(\varphi ^{-1}(a))\, \mathrm{Jac}(\phi ^{-1}(b))|}. \end{aligned}
The other formula for $$K_{H_*}$$ follows from this last one, using that
\begin{aligned} \mathrm {Jac}(\phi )(\phi ^{-1}(a))=\mathrm {Jac}(\phi ^{-1})(a)^{-1}. \end{aligned}
$$\square$$

### 5.2 Proof of Lemma 3.2

From Proposition 2.5, $$\mathfrak {X}_*^{(r,d)}$$ has reproducing kernel
\begin{aligned} K_*^{(r,d)}(p,q) = \frac{K(\psi _d^{-1}(p), \psi _d^{-1}(q))}{\sqrt{|\mathrm{Jac}(\psi _d)(\psi _d^{-1}(p)) \mathrm{Jac}(\psi _d)(\psi _d^{-1}(q))|}}. \end{aligned}
The Jacobian of $$\psi _d$$ is
\begin{aligned} \mathrm{Jac}(\psi _d)(z) = \left( \frac{1}{1 + ||z||^{2}} \right) ^{d+1}. \end{aligned}
(11)
We thus have (writing $$p=(1,z)$$ and $$q=(1,w)$$):
\begin{aligned} \left| K_*^{(r,d)}(p,q) \right| =&\frac{ \frac{r d!}{\pi ^{d}} \frac{ \left| 1 + \left\langle \psi ^{-1}(p), \psi ^{-1}(q) \right\rangle \right| ^{L} }{ \left( 1 + ||\psi ^{-1}(p)||^{2} \right) ^{\frac{d+L+1}{2}} \left( 1 + ||\psi ^{-1}(q)||^{2} \right) ^{\frac{d+L+1}{2}} } }{ \left( \frac{1}{1 + ||\psi ^{-1}(p)||^{2}} \right) ^{\frac{d+1}{2}} \left( \frac{1}{1 + ||\psi ^{-1}(q)||^{2}} \right) ^{\frac{d+1}{2}} }\\ =&\frac{r d!}{\pi ^{d}} \frac{\left| 1 + \left\langle z,w \right\rangle \right| ^{L}}{(1 + \Vert z\Vert ^{2})^{\frac{L}{2}} (1 + \Vert w\Vert ^{2})^{\frac{L}{2}}}\\ =&\frac{r d!}{\pi ^{d}} \frac{\left| \left\langle p,q \right\rangle \right| ^{L}}{\Vert p\Vert ^{L} \Vert q\Vert ^{L}}, \end{aligned}
and the lemma follows. $$\square$$

### 5.3 Proof of Theorem 3.3

Let J be the quantity we want to compute. Following Proposition 2.3, we have that
\begin{aligned} J= & {} \mathrm{E}_{\mathfrak {X}_{*}^{(r,d)}}\left[ \sum _{i \ne j} \frac{1}{\sin \left( d_{\mathbb {P}(\mathbb {C}^{d+1})} (x_{i}, x_{j}) \right) ^{s}} \right] \\= & {} \int _{\mathbb {P}(\mathbb {C}^{d+1})\times \mathbb {P}(\mathbb {C}^{d+1})} \frac{K(p,p)^{2} - |K(p,q)|^{2}}{\sin \left( d_{\mathbb {P}(\mathbb {C}^{d+1})} (p, q) \right) ^{s}} \mathrm{d}p \mathrm{d}q\\= & {} \frac{r^{2} d!^{2} }{\pi ^{2d}}\int _{\mathbb {P}(\mathbb {C}^{d+1})\times \mathbb {P}(\mathbb {C}^{d+1})} \frac{1 - \left| \left\langle p,q \right\rangle \right| ^{2L} }{\left( 1 - \left| \left\langle p,q \right\rangle \right| ^{2}\right) ^{\frac{s}{2}}} \mathrm{d}p \mathrm{d}q, \end{aligned}
where we choose unit norm representatives pq. Since the integrand only depends on the distance between p and q and $$\mathbb {P}(\mathbb {C}^{d+1})$$ is a homogeneous space, we can fix $$p=e_1=(1,0,\ldots ,0)$$ to get
\begin{aligned} J=\frac{r^{2} d! }{\pi ^{d}} \int _{\mathbb {P}(\mathbb {C}^{d+1})} \frac{ 1 - \left| \left\langle e_{1},q \right\rangle \right| ^{2L} }{\left( 1 - \left| \left\langle e_{1},q \right\rangle \right| ^{2}\right) ^{\frac{s}{2}}} \mathrm{d}q, \end{aligned}
where we have used that the volume of $$\mathbb {P}(\mathbb {C}^{d+1})$$ is equal to $${\pi ^{d}}/{d! }$$. In order to compute this integral, we use the change of variables theorem with the map $$\psi _d$$ whose Jacobian is given in (11), getting
\begin{aligned} \begin{aligned} J&= \frac{r^{2} d! }{\pi ^{d}} \int _{\mathbb {C}^{d}} \frac{ 1 - \left| \left\langle e_{1},\frac{(1,z)}{\sqrt{1 + ||z||^{2}}} \right\rangle \right| ^{2L} }{\left( 1 - \left| \left\langle e_{1},\frac{(1,z)}{\sqrt{1 + ||z||^{2}}} \right\rangle \right| ^{2}\right) ^{\frac{s}{2}}} \frac{1}{(1 + ||z||^{2})^{d+1}} \mathrm{d}z \\&= \frac{r^{2} d! }{\pi ^{d}} \int _{\mathbb {C}^d} \frac{ 1 - \left( \frac{1}{1 + ||z||^{2}} \right) ^{L} }{\left( 1 - \frac{1}{1 + ||z||^{2}}\right) ^{\frac{s}{2}}} \left( \frac{1}{1 + ||z||^{2}}\right) ^{d+1} \mathrm{d}z. \\ \end{aligned} \end{aligned}
Integrating in polar coordinates,
\begin{aligned} \begin{aligned} J&= \frac{r^{2} d! }{\pi ^{d}} \frac{2\pi ^{d}}{(d-1)!} \int _{0}^{\infty } \frac{ 1 - \left( \frac{1}{1 + t^{2}} \right) ^{L} }{\left( 1 - \frac{1}{1 + t^{2}}\right) ^{\frac{s}{2}}} \left( \frac{1}{1 + t^{2}}\right) ^{d+1} t^{2d-1} \mathrm{d}t \\&= 2r^{2}d \left[ \int _{0}^{\infty } \frac{ t^{2d-1-s} }{(1 + t^{2})^{d + 1 - \frac{s}{2}}} \mathrm{d}t - \int _{0}^{\infty } \frac{ t^{2d-1-s} }{(1 + t^{2})^{d + 1 - \frac{s}{2} + L}} \mathrm{d}t \right] \\&= 2r^{2}d \left[ \frac{B \left( d - \frac{s}{2}, 1 \right) }{2} - \frac{B \left( d - \frac{s}{2}, L + 1 \right) }{2} \right] \\&= \frac{d}{d - \frac{s}{2}}r^{2} - r^{2}dB \left( d - \frac{s}{2}, L + 1 \right) , \end{aligned} \end{aligned}
as claimed. For the asymptotics, note that for $$L\rightarrow \infty$$ (equiv. $$r\rightarrow \infty$$),
\begin{aligned} B \left( d - \frac{s}{2}, L + 1 \right) =\frac{\Gamma \left( d - \frac{s}{2}\right) \Gamma (L+1)}{\Gamma \left( d - \frac{s}{2}+ L + 1 \right) }\sim \Gamma \left( d - \frac{s}{2}\right) L^{\frac{s}{2}-d},\quad r=\left( {\begin{array}{c}L+d\\ d\end{array}}\right) \sim \frac{L^d}{d!}, \end{aligned}
and hence
\begin{aligned} B \left( d - \frac{s}{2}, L + 1 \right) \sim \Gamma \left( d - \frac{s}{2}\right) (d!r)^{\frac{s}{2d}-1}. \end{aligned}
The asymptotic expansion claimed in the theorem follows. $$\square$$

### 5.4 Proof of Corollary 3.4

Note that $$\mathscr {E}_0(\omega _r)= \left. \frac{d}{ds}\right| _{s=0}\mathscr {E}_s(\omega _r)$$. In particular, interchanging the order of expected value and derivative (it is an exercise to check that this change is justified), from Theorem 3.3 we have
\begin{aligned} \mathrm{E}_{\mathfrak {X}_{*}^{(r,d)}}\left[ \mathscr {E}_{0}^{\mathbb {P}}(\omega _{r}) \right] = \left. \frac{d}{ds} \right| _{s=0}\left( \frac{d}{d - \frac{s}{2}}r^{2} - r^{2}dB \left( d - \frac{s}{2}, L + 1 \right) \right) . \end{aligned}
The proof of the corollary is now a straightforward computation of that derivative, and it is left to the reader. It is helpful to recall the derivative of Euler’s Beta function in terms of the digamma function $$\psi _0$$ for $$m \in \mathbb {N}$$:
\begin{aligned} \frac{d}{dt}B(t,m)=&\frac{d}{dt}\frac{\Gamma (t)\Gamma (m)}{\Gamma (t+m)}\\=&\frac{\Gamma '(t)\Gamma (m)\Gamma (t+m)-\Gamma (t)\Gamma (m)\Gamma '(t+m)}{\Gamma (t+m)^2}\\=&\frac{\psi _0(t)\Gamma (t)\Gamma (m)-\Gamma (t)\Gamma (m)\psi _0(t+m)}{\Gamma (t+m)}\\=&B(t,m)(\psi _0(t)-\psi _0(t+m))\\=&-B(t,m)\sum _{j=0}^{m-1}\frac{1}{t+j}. \end{aligned}

### 5.5 Proof of Proposition 4.2

We will use the following equality, valid for $$y\in (-1,1)$$:
\begin{aligned} \int _{0}^{2\pi } \frac{\hbox {d}\theta }{1 - y \cos (\theta )}=\frac{2\pi }{\sqrt{1-y^2}}. \end{aligned}
(12)
See for example [12, 3.792–1], from which the equality above easily follows.
We have to compute
\begin{aligned}&\frac{1}{(2\pi )^{r}} \int _{\theta _{1},\ldots ,\theta _{r} \in [0, 2\pi ]} \mathrm{E}_{\mathfrak {X}_{*}^{(k,L)}}\left[ \mathscr {E}_{2}(y_{1}^{0},\ldots ,y_{1}^{k-1},\ldots ,y_{r}^{0},\ldots ,y_{r}^{k-1})\right] \hbox {d}(\theta _{1},\ldots ,\theta _{r}) \nonumber \\&\quad = \frac{1}{(2\pi )^{r}} \int _{\theta _{1},\ldots ,\theta _{r} \in [0, 2\pi ]} \mathrm{E}_{\mathfrak {X}_{*}^{(k,L)}}\left[ \sum _{i_{1} \ne i_{2}\text { or } j_{1} \ne j_{2}} \frac{1}{\left| \left| y_{i_{1}}^{j_{1}} - y_{i_{2}}^{j_{2}} \right| \right| ^ {2}} \right] \hbox {d}(\theta _{1},\ldots ,\theta _{r}) \nonumber \\&\quad =J_1+J_2, \end{aligned}
(13)
where
\begin{aligned} J_1=&\frac{1}{(2\pi )^{r}} \int _{\theta _{1},\ldots ,\theta _{r} \in [0, 2\pi ]} \mathrm{E}_{\mathfrak {X}_{*}^{(k,L)}}\left[ \sum _{i=1}^{r} \sum _{j_{1} \ne j_{2}} \frac{1}{\left| \left| y_{i}^{j_{1}} - y_{i}^{j_{2}} \right| \right| ^ {2}}\right] \,\hbox {d}(\theta _{1},\ldots ,\theta _{r}),\\ J_2=&\frac{1}{(2\pi )^{r}} \int _{\theta _{1},\ldots ,\theta _{r} \in [0, 2\pi ]}\mathrm{E}_{\mathfrak {X}_{*}^{(k,L)}}\left[ \sum _{j_{1},j_2=0}^{k-1} \sum _{i_{1} \ne i_{2}} \frac{1}{\left| \left| y_{i_{1}}^{j_{1}} - y_{i_{2}}^{j_{2}} \right| \right| ^ {2}} \right] \, \hbox {d}(\theta _{1},\ldots ,\theta _{r}). \end{aligned}
From (8), we have
\begin{aligned} J_1=&\frac{1}{2\pi }\sum _{i=1}^{r}\int _{\theta \in [0, 2\pi ]} \mathrm{E}_{\mathfrak {X}_{*}^{(k,L)}}\left[ \sum _{j_{1} \ne j_{2}} \frac{1}{\left| \left| e^{\mathbf {i}\left( \theta + \frac{2\pi j_1}{k} \right) } x_i - e^{\mathbf {i}\left( \theta + \frac{2\pi j_2}{k} \right) } x_i \right| \right| ^ {2}}\right] \,\hbox {d}\theta . \end{aligned}
Now, the integral does not depend on $$\theta$$ nor on the (unit norm) vector $$x_i\in \mathbb {C}^{n+1}$$, so we actually have that
\begin{aligned} \frac{J_1}{r}=\sum _{j_{1} \ne j_{2}} \frac{1}{\left| e^{\mathbf {i}\frac{2\pi j_1}{k} } - e^{\mathbf {i}\frac{2\pi j_2}{k}} \right| ^ {2}} \end{aligned}
is the 2-energy of the k roots of unity. This quantity has been studied in much more detail than we need in [9, Theorem 1.1]. In particular, we know that it is of the form $$k^3/12+O(k)$$. We thus conclude
\begin{aligned} J_1=\frac{rk^3}{12}+O(rk). \end{aligned}
(14)
We now compute $$J_2$$. Interchanging the order of integration, we have
\begin{aligned} \begin{aligned} J_2&= \mathrm{E}_{\mathfrak {X}_{*}^{(k,L)}}\left[ \sum _{j_{1},j_2=0}^{k-1} \sum _{i_{1} \ne i_{2}} \frac{1}{4\pi ^{2}}\int _{0}^{2\pi } \int _{0}^{2\pi } \frac{\hbox {d}\theta _{i_{1}} \hbox {d}\theta _{i_{2}} }{\left| \left| e^{\mathbf {i}\left( \theta _{i_{1}} + \frac{2\pi j_{1}}{k} \right) } x_{i_{1}} - e^{\mathbf {i}\left( \theta _{i_{2}} + \frac{2\pi j_{2}}{k} \right) } x_{i_{2}} \right| \right| ^ {2}} \right] , \end{aligned} \end{aligned}
where we can choose whatever unit norm representatives we wish of $$x_{i_1}$$ and $$x_{i_2}$$. In order to compute the inner integral, for any fixed $$i_i,i_2$$, we assume that our choice satisfies $$\langle x_{i_1},x_{i_2}\rangle \in [0,1]$$ (i.e., it is real and non-negative), which readily implies
\begin{aligned} \sin d_{\mathbb {P}(\mathbb {C}^{d+1})}(x_{i_1},x_{i_2}) = \sqrt{1 -\left\langle x_{i_1},x_{i_2}\right\rangle ^{2}}. \end{aligned}
(15)
A simple computation using the invariance of the integral under rotations yields
\begin{aligned}&\frac{1}{4\pi ^{2}}\int _{0}^{2\pi } \int _{0}^{2\pi } \frac{\hbox {d}\theta _{i_{1}} \hbox {d}\theta _{i_{2}} }{\left| \left| e^{\mathbf {i}\left( \theta _{i_{1}} + \frac{2\pi j_{1}}{k} \right) } x_{i_{1}} - e^{\mathbf {i}\left( \theta _{i_{2}} + \frac{2\pi j_{2}}{k} \right) } x_{i_{2}} \right| \right| ^ {2}}\\&\quad =\frac{1}{2\pi }\int _0^{2\pi }\frac{\hbox {d}\theta }{2-2\left\langle x_{i_1},x_{i_2}\right\rangle \cos \theta }{\mathop {=}\limits ^{(12)}}\frac{1}{2\sqrt{1-\left\langle x_{i_1},x_{i_2}\right\rangle ^2}}{\mathop {=}\limits ^{(15)}}\frac{1}{2\sin d_{\mathbb {P}(\mathbb {C}^{d+1})}(x_{i_1},x_{i_2})}, \end{aligned}
and this last value is independent of $$j_1,j_2$$. We thus have
\begin{aligned} J_2= \frac{k^2}{2}\mathrm{E}_{\mathfrak {X}_{*}^{(k,L)}}\left[ \sum _{i_{1} \ne i_{2}} \frac{1}{\sin d_{\mathbb {P}(\mathbb {C}^{d+1})}(x_{i_1},x_{i_2})}\right] . \end{aligned}
This last expected value has been computed in Theorem 3.3, which yields
\begin{aligned} J_2= \frac{d}{2d-1} (kr)^{2}-\frac{d\Gamma \left( d-\frac{1}{2}\right) }{2(d!)^{1-\frac{1}{2d}}} k^2r^{1+\frac{1}{2d}}+o\left( k^2r^{1+\frac{1}{2d}}\right) . \end{aligned}
(16)
Proposition 4.2 follows from (13), (14), and (16). $$\square$$

### 5.6 Proof of Theorem 1.2

Fix $$d\ge 1$$, and let
\begin{aligned} f(A)=\frac{A^{2 - \frac{2}{2d+1}} }{12} -\frac{d \Gamma \left( d - \frac{1}{2} \right) A^{1 - \frac{2}{2d+1}} }{2 \left( d!\right) ^{1 - \frac{1}{2d}} } \end{aligned}
be the coefficient of $$n^{1+\frac{2}{2d+1}}$$ in (10). The function f(A) has a strict global minimum at
\begin{aligned} A_d=\frac{3 \Gamma \left( d - \frac{1}{2} \right) (2d-1)}{2 \left( d!\right) ^{1 - \frac{1}{2d}} }. \end{aligned}
Indeed,
\begin{aligned} f(A_d)=-\frac{3^{1 - \frac{2}{2d+1}} (2d-1)^{1 - \frac{2}{2d+1}} (2d+1) \Gamma \left( d- \frac{1}{2} \right) ^{2 - \frac{2}{2d+1}}}{2^{4 - \frac{2}{2d+1}} (d!)^{2 - \frac{4}{2d+1}}} \end{aligned}
gives the bound for the $$\limsup$$ given in Theorem 1.2. We cannot just let $$k=A_dr^{\frac{1}{2d}}$$ in Corollary 4.3 since it might happen that $$k\not \in \mathbb {Z}$$, but we will easily deal with this problem. Let $$L\ge 1$$ be any positive integer, let $$r=\left( {\begin{array}{c}d+L\\ d\end{array}}\right)$$, and let A be the unique number in the interval
\begin{aligned} \big [A_d,A_d+r^{-\frac{1}{2d}}\big ) \end{aligned}
such that $$k=Ar^{\frac{1}{2d}}\in \mathbb {Z}$$. Finally, let $$n=n_L=rk$$, which depends uniquely on d and L, and which satisfies $$n_L\rightarrow \infty$$ as $$L\rightarrow \infty$$. For any $$\epsilon >0$$, we then have
\begin{aligned} \limsup _{L\rightarrow \infty }\frac{ V_{2}(\mathbb {S}^{2d+1})n_L^{2}-\min _{\omega _{n_L}}\left( \mathscr {E}_{2}(\omega _{n_L})\right) }{n_L^{1+\frac{2}{2d+1}}} \ge -f(A)\ge -f(A_d)-\epsilon , \end{aligned}
the first inequality from Corollary 4.3 and the second inequality due to $$r\rightarrow \infty$$ as $$L\rightarrow \infty$$, which implies for some constant $$C>0$$:
\begin{aligned} |f(A)-f(A_d)| \le Cr^{-\frac{1}{2d}}\rightarrow 0,\quad L\rightarrow \infty . \end{aligned}
We have thus proved
\begin{aligned} \limsup _{L\rightarrow \infty }\frac{ V_{2}(\mathbb {S}^{2d+1})n_L^{2}-\min _{\omega _{n_L}}\left( \mathscr {E}_{2}(\omega _{n_L})\right) }{n_L^{1+\frac{2}{2d+1}}} \ge -f(A_d), \end{aligned}
which finishes the proof of our Theorem 1.2. $$\square$$

### 5.7 Proof of Theorem 1.3

From [3], the Green function of $$\mathbb {P}(\mathbb {C}^{d+1})$$ is given by $$G(x,y)=\phi (r)$$, where $$r=d_{\mathbb {P}(\mathbb {C}^{d+1})}(x,y)$$ and
\begin{aligned} \phi '(r)=-\frac{1}{Vol(\mathbb {P}(\mathbb {C}^{d+1}))}\frac{\int _r^{\pi /2}\sin ^{2d-1}t\cos t\,\hbox {d}t}{\sin ^{2d-1}r\cos r}=-\frac{1}{2dVol(\mathbb {P}(\mathbb {C}^{d+1}))}\frac{1-\sin ^{2d}r}{\sin ^{2d-1}r\cos r}. \end{aligned}
Integrating the formula above (see for example [12, 2.517–1]), we have
\begin{aligned} \begin{aligned} \phi (r) =&\frac{1}{2dVol(\mathbb {P}(\mathbb {C}^{d+1}))} \left[ \frac{1}{2} \displaystyle \sum _{k=1}^{d-1} \frac{1}{(d-k) \left( \sin r \right) ^{2d-2k}} - \log \left( \sin r \right) \right] +C. \end{aligned} \end{aligned}
In order to compute the constant, we need to impose that the average of $$G(x,\cdot )$$ equals 0 for all (i.e., for some) $$x\in \mathbb {P}(\mathbb {C}^{d+1})$$. Let $$x=(1,0)$$, and change variables using $$\psi _d$$ from Lemma 3.2 whose Jacobian is given in (11) to compute
\begin{aligned} C= & {} - \frac{1}{2dVol(\mathbb {P}(\mathbb {C}^{d+1}))^2} \left[ \frac{1}{2} \displaystyle \sum _{k=1}^{d-1} \int _{z\in \mathbb {C}^d}\frac{(1+\Vert z\Vert ^2)^{-k-1}}{(d-k) \Vert z\Vert ^{2d-2k}} \,\hbox {d}z \right. \\&\left. \quad - \frac{1}{2}\int _{z\in \mathbb {C}^d}\frac{\log \left( \frac{\Vert z\Vert ^2}{1+\Vert z\Vert ^2} \right) }{(1+\Vert z\Vert ^2)^{d+1}}\,\hbox {d}z \right] . \end{aligned}
Integrating in polar coordinates,
\begin{aligned} C=&\frac{1}{2Vol(\mathbb {P}(\mathbb {C}^{d+1}))}\left( \int _{0}^\infty \frac{t^{2d-1}\log \left( \frac{t^2}{1+t^2} \right) }{(1+t^2)^{d+1}}\,\hbox {d}t\right. \\&\left. -\, \displaystyle \sum _{k=1}^{d-1} \int _{0}^\infty \frac{t^{2k-1}}{(d-k)(1+t^2)^{k+1}} \,\hbox {d}t\right) \\ =&-\frac{d!}{4\pi ^d}\left( \frac{1}{d^{2}} + \displaystyle \sum _{k=1}^{d-1} \frac{1}{k(d-k)}\right) \\=&-\frac{(d-1)!}{4\pi ^d}\left( \frac{1}{d}+2\sum _{k=1}^{d-1}\frac{1}{k}\right) . \end{aligned}
For the computation of the integrals, we have used the change of variables $$s=t^2/(1+t^2)$$ and [12, 4.272–6].
We thus conclude for $$r=d_{\mathbb {P}(\mathbb {C}^{d+1})}(x,y)$$:
\begin{aligned} \begin{aligned} G(x,y) =&\frac{(d-1)!}{2\pi ^{d}} \left[ \left( \frac{1}{2} \displaystyle \sum _{k=1}^{d-1} \frac{1}{(d-k) \left( \sin r \right) ^{2d-2k}} \right) - \log \left( \sin r\right) \right] \\&-\frac{(d-1)!}{4\pi ^d}\left( \frac{1}{d}+2\sum _{k=1}^{d-1}\frac{1}{k}\right) . \end{aligned} \end{aligned}
Following the definitions of Theorem 3.3 and Corollary 3.4, the expected value of Green energy may be expressed as
\begin{aligned}&\mathrm{E}_{\mathfrak {X}_{*}^{(r,d)}}\left[ \mathscr {E}_{G}^{\mathbb {P}}(\omega _{r})\right] \\&\quad = \overbrace{\frac{(d-1)!}{2\pi ^{d}} \left[ \left( \frac{1}{2} \displaystyle \sum _{k=1}^{d-1} \frac{1}{d-k} \mathrm{E}_{\mathfrak {X}_{*}^{(r,d)}}\left[ \mathscr {E}_{2d-2k}^{\mathbb {P}}(\omega ) \right] \right) + \mathrm{E}_{\mathfrak {X}_{*}^{(r,d)}}\left[ \mathscr {E}_{0}^{\mathbb {P}}(\omega ) \right] \right] }^{A} \\&\qquad -\frac{r(r-1)(d-1)!}{4\pi ^d}\left( \frac{1}{d}+2\sum _{k=1}^{d-1}\frac{1}{k}\right) . \\ \end{aligned}
Each of the expected values in the last expression has been computed in Theorem 3.3 and Corollary 3.4, producing
\begin{aligned} A= & {} \frac{(d-1)!}{4\pi ^{d}} \left[ \left( \displaystyle \sum _{k=1}^{d-1} \frac{1}{d-k} \left( \frac{d}{k}r^{2}-r^{2-\frac{k}{d}}\frac{d \Gamma \left( k\right) }{(d!)^{\frac{k}{d}}} \right) \right) + \frac{r^2}{d} + \frac{r\log r}{d} \right] +o\left( r^{2-\frac{1}{d}}\right) \\= & {} r^{2} \frac{d!}{4\pi ^{d}} \left( \sum _{k=1}^{d-1} \frac{1}{k(d-k)} + \frac{1}{d^2} \right) - \frac{(d!)^{1- \frac{1}{d}}}{4\pi ^{d}(d-1)} r^{2 - \frac{1}{d}} +o\left( r^{2-\frac{1}{d}}\right) \\= & {} r^{2} \frac{(d-1)!}{4\pi ^{d}} \left( \frac{1}{d}+2\sum _{k=1}^{d-1} \frac{1}{k} \right) - \frac{(d!)^{1- \frac{1}{d}}}{4\pi ^{d}(d-1)} r^{2 - \frac{1}{d}} +o\left( r^{2-\frac{1}{d}}\right) . \end{aligned}
We thus have
\begin{aligned} \begin{aligned} \mathrm{E}_{\mathfrak {X}_{*}^{(r,d)}}\left[ \mathscr {E}_{G}^{\mathbb {P}}(\omega _{r})\right]&= - \frac{(d!)^{1- \frac{1}{d}}}{4\pi ^{d}(d-1)} r^{2 - \frac{1}{d}} +o\left( r^{2-\frac{1}{d}}\right) . \end{aligned} \end{aligned}
Since this last equation holds for an infinite sequence of numbers (those of the form $$r=\left( {\begin{array}{c}d+L\\ d\end{array}}\right)$$), Theorem 1.3 follows.

## References

1. 1.
Alishahi, K., Zamani, M.: The spherical ensemble and uniform distribution of points on the sphere. Electron. J. Probab. 20, 23–27 (2015)
2. 2.
Beltrán, C., Marzo, J., Ortega-Cerdà, J.: Energy and discrepancy of rotationally invariant determinantal point processes in high dimensional spheres. J. Complexity 37, 76–109 (2016)
3. 3.
Beltrán, C., Corral, N., Criado del Rey, J.G.: Discrete and continuous green energy on compact manifolds. arXiv:1702.00864 [math.DG]
4. 4.
Berman, R.J.: Determinantal point processes and fermions on complex manifolds: large deviations and bosonization. Commun. Math. Phys. 327(1), 1–47 (2014)
5. 5.
Bétermin, L., Sandier, E.: Renormalized energy and asymptotic expansion of optimal logarithmic energy on the sphere. Constr. Approx. 47(1), 39–74 (2018)
6. 6.
Borodachov, S.V., Hardin, D.P., Saff, E.B.: Minimal Discrete Energy on the Sphere and Other Manifolds. Springer, Berlin (to appear)Google Scholar
7. 7.
Brauchart, J.S.: About the second term of the asymptotics for optimal Riesz energy on the sphere in the potential-theoretical case. Integr. Transforms Spec. Funct. 17(5), 321–328 (2006)
8. 8.
Brauchart, J.S., Grabner, P.J.: Distributing many points on spheres: minimal energy and designs. J. Complexity 31(3), 293–326 (2015)
9. 9.
Brauchart, J.S., Hardin, D.P., Saff, E.B.: The Riesz energy of the Nth roots of unity: an asymptotic expansion for large N. Bull. Lond. Math. Soc. 41(4), 621–633 (2009).
10. 10.
Brauchart, J.S., Hardin, D.P., Saff, E.B.: The next-order term for optimal Riesz and logarithmic energy asymptotics on the sphere. In: Recent Advances in Orthogonal Polynomials, Special Functions, and Their Applications, pp. 31–61 (2012). https://doi.org/10.1090/conm/578/11483
11. 11.
Doohovskoy, A.P., Landkof, N.S.: Foundations of Modern Potential Theory. Grundlehren der mathematischen Wissenschaften. Springer, Berlin (2011)Google Scholar
12. 12.
Gradshteyn, I.S., Ryzhik, I.M.: Table of integrals, series, and products, 8th edn. Elsevier /Academic Press, Amsterdam (2015) (Translated from the Russian, Translation edited and with a preface by Daniel Zwillinger and Victor Moll, Revised from the seventh edition)Google Scholar
13. 13.
Hough, J.B., Krishnapur, M., Peres, Y., Virág, B.: Zeros of Gaussian Analytic Functions and Determinantal Point Processes, University Lecture Series, vol. 51. American Mathematical Society, Providence, RI (2009)
14. 14.
Krishnapur, M.: From random matrices to random analytic functions. Ann. Probab. 37(1), 314–346 (2009)
15. 15.
Kuijlaars, A.B.J., Saff, E.B.: Asymptotics for minimal discrete energy on the sphere. Trans. Am. Math. Soc. 350(2), 523–538 (1998)
16. 16.
Macchi, O.: The coincidence approach to stochastic point processes. Adv. Appl. Probab. 7, 83–122 (1975)
17. 17.
Rakhmanov, E.A., Saff, E.B., Zhou, Y.M.: Minimal discrete energy on the sphere. Math. Res. Lett. 1(6), 647–662 (1994)
18. 18.
Sandier, E., Serfaty, S.: 2D Coulomb gases and the renormalized energy. Ann. Probab. 43(4), 2026–2083 (2015)
19. 19.
Scardicchio, A., Zachary, C.E., Torquato, S.: Statistical properties of determinantal point processes in high-dimensional Euclidean spaces. Phys. Rev. E 79, 041108 (2009).
20. 20.
Soshnikov, A.: Determinantal random point fields. Uspekhi Mat. Nauk 55(5–335), 107–160 (2000)