Random organization and non-equilibrium hyperuniform fluids on a sphere

Randomly organizing hyperuniform fluid induced by reciprocal activation is a non-equilibrium fluid with vanishing density fluctuations at large length scales such as crystals. Here, we extend this new state of matter to a closed manifold, namely a spherical surface. We find that the random organizat...

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Main Authors: Lei, Yusheng, Zheng, Ning, Ni, Ran
Other Authors: School of Chemistry, Chemical Engineering and Biotechnology
Format: Article
Language:English
Published: 2023
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Online Access:https://hdl.handle.net/10356/171427
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Institution: Nanyang Technological University
Language: English
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spelling sg-ntu-dr.10356-1714272023-10-27T15:31:51Z Random organization and non-equilibrium hyperuniform fluids on a sphere Lei, Yusheng Zheng, Ning Ni, Ran School of Chemistry, Chemical Engineering and Biotechnology Science::Chemistry Density Fluctuation Directed Percolation Randomly organizing hyperuniform fluid induced by reciprocal activation is a non-equilibrium fluid with vanishing density fluctuations at large length scales such as crystals. Here, we extend this new state of matter to a closed manifold, namely a spherical surface. We find that the random organization on a spherical surface behaves similar to that in two dimensional Euclidean space, and the absorbing transition on a sphere also belongs to the conserved directed percolation universality class. Moreover, the reciprocal activation can also induce a non-equilibrium hyperuniform fluid on a sphere. The spherical structure factor at the absorbing transition and the non-equilibrium hyperuniform fluid phases are scaled as S(l → 0) ∼ (l/R)0.45 and S(l → 0) ∼ l(l + 1)/R2, respectively, which are both hyperuniform according to the definition of hyperuniformity on a sphere with l, the wave number, and R, the radius of the spherical surface. We also consider the impact of inertia in realistic hyperuniform fluids, and it is found only by adding an extra length-scale, above which hyperuniform scaling appears. Our finding suggests a new method for creating non-equilibrium hyperuniform fluids on closed manifolds to avoid boundary effects. Ministry of Education (MOE) Published version This work has been supported by the Singapore Ministry of Education through the Academic Research Fund No. MOE2019-T2-2-010. 2023-10-24T07:33:35Z 2023-10-24T07:33:35Z 2023 Journal Article Lei, Y., Zheng, N. & Ni, R. (2023). Random organization and non-equilibrium hyperuniform fluids on a sphere. Journal of Chemical Physics, 159(8), 081101-1-081101-6. https://dx.doi.org/10.1063/5.0165527 0021-9606 https://hdl.handle.net/10356/171427 10.1063/5.0165527 37606337 2-s2.0-85168460417 8 159 081101-1 081101-6 en MOE2019-T2-2-010 Journal of Chemical Physics © 2023 Author(s). Published under an exclusive license by AIP Publishing. All rights reserved. This article may be downloaded for personal use only. Any other use requires prior permission of the copyright holder. The Version of Record is available online at http://doi.org/10.1063/5.0165527 application/pdf
institution Nanyang Technological University
building NTU Library
continent Asia
country Singapore
Singapore
content_provider NTU Library
collection DR-NTU
language English
topic Science::Chemistry
Density Fluctuation
Directed Percolation
spellingShingle Science::Chemistry
Density Fluctuation
Directed Percolation
Lei, Yusheng
Zheng, Ning
Ni, Ran
Random organization and non-equilibrium hyperuniform fluids on a sphere
description Randomly organizing hyperuniform fluid induced by reciprocal activation is a non-equilibrium fluid with vanishing density fluctuations at large length scales such as crystals. Here, we extend this new state of matter to a closed manifold, namely a spherical surface. We find that the random organization on a spherical surface behaves similar to that in two dimensional Euclidean space, and the absorbing transition on a sphere also belongs to the conserved directed percolation universality class. Moreover, the reciprocal activation can also induce a non-equilibrium hyperuniform fluid on a sphere. The spherical structure factor at the absorbing transition and the non-equilibrium hyperuniform fluid phases are scaled as S(l → 0) ∼ (l/R)0.45 and S(l → 0) ∼ l(l + 1)/R2, respectively, which are both hyperuniform according to the definition of hyperuniformity on a sphere with l, the wave number, and R, the radius of the spherical surface. We also consider the impact of inertia in realistic hyperuniform fluids, and it is found only by adding an extra length-scale, above which hyperuniform scaling appears. Our finding suggests a new method for creating non-equilibrium hyperuniform fluids on closed manifolds to avoid boundary effects.
author2 School of Chemistry, Chemical Engineering and Biotechnology
author_facet School of Chemistry, Chemical Engineering and Biotechnology
Lei, Yusheng
Zheng, Ning
Ni, Ran
format Article
author Lei, Yusheng
Zheng, Ning
Ni, Ran
author_sort Lei, Yusheng
title Random organization and non-equilibrium hyperuniform fluids on a sphere
title_short Random organization and non-equilibrium hyperuniform fluids on a sphere
title_full Random organization and non-equilibrium hyperuniform fluids on a sphere
title_fullStr Random organization and non-equilibrium hyperuniform fluids on a sphere
title_full_unstemmed Random organization and non-equilibrium hyperuniform fluids on a sphere
title_sort random organization and non-equilibrium hyperuniform fluids on a sphere
publishDate 2023
url https://hdl.handle.net/10356/171427
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