2018
DOI: 10.1103/physreve.97.010102
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Disordered multihyperuniformity derived from binary plasmas

Abstract: Disordered multihyperuniform many-particle systems are exotic amorphous states that allow exquisite color sensing capabilities due to their anomalous suppression of density fluctuations for distinct subsets of particles, as recently evidenced in photoreceptor mosaics in avian retina. Motivated by this biological finding, we present a statistical-mechanical model that rigorously achieves disordered multihyperuniform many-body systems by tuning interactions in binary mixtures of nonadditive hard-disk plasmas. We… Show more

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Cited by 15 publications
(41 citation statements)
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“…All crystals [27], many quasicrystals [32,33], stealthy and other hyperuniform disordered ground states [62,63,65,68,143], perturbed lattices [134,[137][138][139]145], g 2 -invariant disordered point processes [27], one-component plasmas [35,146], hard-sphere plasmas [147,148], random organization models [56], perfect glasses [68], and Weyl-Heisenberg ensembles [136].…”
Section: Class Modelsmentioning
confidence: 99%
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“…All crystals [27], many quasicrystals [32,33], stealthy and other hyperuniform disordered ground states [62,63,65,68,143], perturbed lattices [134,[137][138][139]145], g 2 -invariant disordered point processes [27], one-component plasmas [35,146], hard-sphere plasmas [147,148], random organization models [56], perfect glasses [68], and Weyl-Heisenberg ensembles [136].…”
Section: Class Modelsmentioning
confidence: 99%
“…where ρ i is the number density of type-i particles, respectively, and ρ is the total number density. Substitution of (148) into (145), (146) and (147) yields the corresponding packing fraction, autocovariance function and spectral density,…”
Section: Spectral Densities For Packingsmentioning
confidence: 99%
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“…However, multicomponent equilibrium plasmas consisting of nonadditive hard spheres with Coulombic interactions enable one to generate a very wide class of disordered hyperuniform as well as "multihyperuniform" 27 systems at positive temperatures. 199,200…”
Section: Equilibrium and Metastable Behaviormentioning
confidence: 99%
“…σ 2 * n (s) ∝ p * δ with δ < 2, and δ decreasing as the interaction range increases. In fact, for the Coulomb like interaction we have δ ≈ 1.4 Note the this interaction gives strictly δ = 1 for planar surfaces [30]. The pure LJ fluid, as in the Euclidean case, displays no hyperuniformity, and conforms to the same scaling as the uniform random point patterns.…”
Section: Number Variances In Fluids Of Interacting Particlesmentioning
confidence: 82%