Abstract:In this paper we study Riesz, Green and logarithmic energy on two-point homogeneous spaces. More precisely we consider the real, the complex, the quaternionic and the Cayley projective spaces. For each of these spaces we provide upper estimates for the mentioned energies using determinantal point processes. Moreover, we determine lower bounds for these energies of the same order of magnitude.
“…Our main new result is the following lower bound for the Green energy on S n . Note that similar results are known for the Green energy in projective spaces [1]. Theorem 4.2 (Main result).…”
Section: A Lower Bound For the Green Energy On S Nsupporting
confidence: 55%
“…where G(M; •, •) is the Green function in M associated to the Laplace-Beltrami operator, is a more natural choice since it does not depend on extrinsic quantities, and is attracting more attention in the last few years, see [13], [20], [1]. It turns out that the Green function in S 2 is…”
Section: The Green Function In S Nmentioning
confidence: 99%
“…The Green function of a general Riemannian manifold can be very hard to compute. In [4], a method is given to compute it in compact harmonic manifolds, that is to say, in spheres and projective spaces (see [1] for an alternative, equivalent method). We have used it to get the explicit expression of G(S n ; p, q) in Proposition 3.1.…”
Section: Appendix a Some Special Functionsmentioning
We show an alternative proof of the sharpest known lower bound for the logarithmic energy on the unit sphere S 2 . We then generalize this proof to get new lower bounds for the Green energy on the unit n-sphere S n .
“…Our main new result is the following lower bound for the Green energy on S n . Note that similar results are known for the Green energy in projective spaces [1]. Theorem 4.2 (Main result).…”
Section: A Lower Bound For the Green Energy On S Nsupporting
confidence: 55%
“…where G(M; •, •) is the Green function in M associated to the Laplace-Beltrami operator, is a more natural choice since it does not depend on extrinsic quantities, and is attracting more attention in the last few years, see [13], [20], [1]. It turns out that the Green function in S 2 is…”
Section: The Green Function In S Nmentioning
confidence: 99%
“…The Green function of a general Riemannian manifold can be very hard to compute. In [4], a method is given to compute it in compact harmonic manifolds, that is to say, in spheres and projective spaces (see [1] for an alternative, equivalent method). We have used it to get the explicit expression of G(S n ; p, q) in Proposition 3.1.…”
Section: Appendix a Some Special Functionsmentioning
We show an alternative proof of the sharpest known lower bound for the logarithmic energy on the unit sphere S 2 . We then generalize this proof to get new lower bounds for the Green energy on the unit n-sphere S n .
“…where G(M; •, •) is the Green function in M associated to the Laplace-Beltrami operator, is a more natural choice since it does not depend on extrinsic quantities, and is attracting more attention in the last few years, see [1,14,23]. It turns out that the Green function in S 2 is…”
We show an alternative proof of the sharpest known lower bound for the logarithmic energy on the unit sphere $$\mathbb {S}^2$$
S
2
. We then generalize this proof to get new lower bounds for the Green energy on the unit n-sphere $$\mathbb {S}^n$$
S
n
.
“…The second property implies that the random points exhibit some repulsion, and has been used to give upper bounds on the minimum value of the energy E log (K, n) (and other energies) for different sets: in [2] for the 2-sphere S 2 , in [7] for the d-sphere S d , in [5] (see also [8]) for the complex projective space, in [3] for 2-point homogeneous spaces, in [18] for the flat torus and in [6] for the rotation group SO (3).…”
In this paper we compute the logarithmic energy of points in the unit interval [-1,1] chosen from different Gegenbauer Determinantal Point Processes. We check that all the different families of Gegenbauer polynomials yield the same asymptotic result to third order, we compute exactly the value for Chebyshev polynomials and we give a closed expression for the minimal possible logarithmic energy. The comparison suggests that DPPs cannot match the value of the minimum beyond the third asymptotic term.
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