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Statistical properties of determinantal point processes in high ...

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SCARDICCHIO, ZACHARY, AND TORQUATO PHYSICAL REVIEW E 79, 041108 2009<br />

M * (s)<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

d=1<br />

d=2<br />

d=3<br />

d=4<br />

0<br />

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5<br />

s=r/λ<br />

statistics <strong>in</strong> dimensions one to four. Our results strongly suggest<br />

that both G P and G V are l<strong>in</strong>ear for sufficiently large r,<br />

and we obta<strong>in</strong> numerical estimates <strong>of</strong> the common slope <strong>in</strong><br />

this limit. This behavior is to be contrasted with the equivalent<br />

forms <strong>of</strong> G P and G V for equilibrium systems <strong>of</strong> hard<br />

spheres and for Poisson <strong>po<strong>in</strong>t</strong> <strong>processes</strong>. It is known for the<br />

former systems that both functions saturate for sufficiently<br />

large r while G Pr=G Vr=1 for all r <strong>in</strong> the latter <strong>processes</strong><br />

2. The l<strong>in</strong>earity <strong>of</strong> G P and G V <strong>in</strong> the <strong>determ<strong>in</strong>antal</strong> case is<br />

thus unique <strong>in</strong> the context <strong>of</strong> general <strong>po<strong>in</strong>t</strong> <strong>processes</strong>. We<br />

have also shown, <strong>in</strong> accordance with 6, that <strong>in</strong> the limit as<br />

d→ both G P and G V must saturate at unity <strong>in</strong> accordance<br />

with the behavior <strong>of</strong> the aforementioned bounds; aga<strong>in</strong>, this<br />

claim is supported by the numerical evidence we have presented<br />

here. Also, as the dimension d grows, we observed<br />

that the functions H P and H V become concentrated around<br />

their maximum as do the distributions <strong>of</strong> extrema <strong>of</strong> nearestneighbor<br />

distances M * and M*.<br />

M * (s)<br />

4<br />

3<br />

2<br />

1<br />

d=1<br />

d=2<br />

d=3<br />

d=4<br />

0<br />

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1<br />

s=r/λ<br />

FIG. 15. Color onl<strong>in</strong>e Distributions <strong>of</strong> the maximum M*s; left and m<strong>in</strong>imum M * s; right nearest-neighbor distances across<br />

dimensions at unit mean nearest-neighbor separation . Results are simulated us<strong>in</strong>g the HKPV algorithm.<br />

4<br />

3.5<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

M<strong>in</strong>imum nearest-neighbor distance<br />

Maximum nearest-neighbor distance<br />

Unit mean nearest-neighbor distance<br />

0<br />

0 1 2 3 4 5<br />

d<br />

FIG. 16. Color onl<strong>in</strong>e Average maxima and m<strong>in</strong>ima nearestneighbor<br />

distances with standard deviations across dimensions at<br />

unit mean nearest-neighbor separation; results are obta<strong>in</strong>ed us<strong>in</strong>g<br />

the HKPV algorithm. Also <strong>in</strong>cluded for reference is the unit mean<br />

nearest-neighbor separation, which is fixed for each dimension.<br />

041108-18<br />

By us<strong>in</strong>g the HKPV algorithm to generate configurations<br />

<strong>of</strong> <strong>po<strong>in</strong>t</strong>s we have shown that the <strong>determ<strong>in</strong>antal</strong> nature <strong>of</strong> the<br />

n-particle probability density has a significant effect on the<br />

Voronoi cell statistics <strong>of</strong> the Fermi-sphere <strong>po<strong>in</strong>t</strong> process <strong>in</strong><br />

two dimensions. Namely, the probability distribution <strong>of</strong> cell<br />

sides is more peaked around n=6 hexagons than the correspond<strong>in</strong>g<br />

distribution for either the Poisson <strong>po<strong>in</strong>t</strong> process or<br />

the G<strong>in</strong>ibre ensemble 38 the distribution <strong>of</strong> complex eigenvalues<br />

<strong>of</strong> random complex matrices. The effective separation<br />

<strong>of</strong> the <strong>po<strong>in</strong>t</strong>s, result<strong>in</strong>g <strong>in</strong> a sharper peak <strong>in</strong> the distribution<br />

<strong>of</strong> the number <strong>of</strong> sides <strong>of</strong> the Voronoi cells, is closely<br />

related to the hyperuniformity <strong>of</strong> the system.<br />

F<strong>in</strong>ally, to show how the algorithm can be used for generat<strong>in</strong>g<br />

<strong>determ<strong>in</strong>antal</strong> <strong>processes</strong> on curved spaces, we have<br />

presented an example <strong>of</strong> a <strong>determ<strong>in</strong>antal</strong> <strong>po<strong>in</strong>t</strong> process on the<br />

two-sphere.<br />

FIG. 17. Color onl<strong>in</strong>e Configuration <strong>of</strong> 37 <strong>po<strong>in</strong>t</strong>s on the unit<br />

sphere us<strong>in</strong>g the HKPB algorithm with the spherical harmonics as<br />

basis functions.

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