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arxiv: 2606.22250 · v1 · pith:5FGZLHOOnew · submitted 2026-06-20 · ❄️ cond-mat.soft · cond-mat.stat-mech

Quasi-two-dimensional dispersions of Brownian particles with competitive interactions: Dynamical clustering, non-Gaussianity and hydrodynamic correlations

Pith reviewed 2026-06-26 10:58 UTC · model grok-4.3

classification ❄️ cond-mat.soft cond-mat.stat-mech
keywords quasi-two-dimensionalBrownian particlescompetitive interactionsdynamical clusteringnon-Gaussianityhydrodynamic interactionsvan Hove function
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The pith

Clustered quasi-two-dimensional particle systems with competing interactions exhibit exponential self-van Hove functions and earlier onset of hydrodynamic interactions.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper analyzes the dynamics of quasi-two-dimensional dispersions of Brownian particles with short-range attractive and long-range repulsive interactions using Langevin dynamics and multiparticle collision dynamics simulations. Strengthening the attractive interaction suppresses self-diffusion and induces subdiffusive behavior through clustering, with cluster lifetimes depending more strongly on attraction strength than on particle concentration. Two dynamical criteria based on mean cluster lifetime and relaxation time of local hexagonal order identify the transition to the clustered phase. In the equilibrium-cluster phase, the self-van Hove function takes an approximately exponential form, indicating non-Gaussian dynamics consistent with a diffusing-diffusivity mechanism. Hydrodynamic interactions are shown to govern collective dynamics, preserving enhanced large-scale collective diffusion while clustering causes these interactions to become relevant on earlier, inertial timescales.

Core claim

Clustered Q2D-SALR systems exhibit pronounced non-Gaussian dynamics. In particular, the self-van Hove function in the equilibrium-cluster phase displays an approximately exponential form, consistent with an underlying diffusing-diffusivity mechanism. MPC simulations reveal the critical role of hydrodynamic interactions in collective dynamics, with clustering leading to an earlier onset of HIs.

What carries the argument

The self-van Hove function, analyzed for its exponential form in the clustered phase, and the time-dependent hydrodynamic function, used to track the onset of hydrodynamic interactions via multiparticle collision dynamics.

Load-bearing premise

The simulation methods faithfully reproduce the physical behavior of the Q2D-SALR system, and the exponential form of the self-van Hove function arises from a diffusing-diffusivity mechanism rather than simulation artifacts.

What would settle it

A direct measurement showing a Gaussian rather than exponential self-van Hove function throughout the equilibrium-cluster phase would contradict the non-Gaussian dynamics claim.

read the original abstract

We conduct a comprehensive dynamical analysis of quasi-two-dimensional (Q2D) dispersions of Brownian particles with competing short-range attractive (SA) and long-range repulsive (LR) interactions using Langevin dynamics (LD) and multiparticle collision dynamics (MPC). As the attractive interaction is strengthened, self-diffusion is significantly suppressed, and clustering gives rise to pronounced subdiffusive behavior. We find that cluster lifetimes are influenced more strongly by attraction strength than by particle concentration. Two dynamical criteria for the transition from non-clustered to clustered phases are identified in terms of the mean cluster lifetime and the relaxation time of local hexagonal order, respectively. Moreover, clustered Q2D-SALR systems exhibit pronounced non-Gaussian dynamics. In particular, the self-van Hove function in the equilibrium-cluster phase displays an approximately exponential form, consistent with an underlying diffusing-diffusivity mechanism. Importantly, MPC simulations reveal the critical role of hydrodynamic interactions (HIs) in collective dynamics. We observe that the anomalously enhanced large-scale collective diffusion characteristic of hydrodynamically interacting Q2D systems is qualitatively preserved in Q2D-SALR dispersions. However, this enhancement suppresses the intermediate-range-order peak in the hydrodynamic function compared to its three-dimensional counterpart. Furthermore, by analyzing the time-dependent evolution of hydrodynamic function and the sound mode in hydrodynamic correlations, we find that clustering in Q2D-SALR systems leads to an earlier onset of HIs than in Q2D hard-sphere reference systems, implying HIs become relevant already on inertial timescales.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 0 minor

Summary. The manuscript reports a simulation study of quasi-two-dimensional Brownian particles with competing short-range attractive and long-range repulsive (SALR) interactions, employing both Langevin dynamics (LD) without hydrodynamics and multiparticle collision dynamics (MPC) with hydrodynamics. Key findings include suppression of self-diffusion and emergence of subdiffusive behavior with increasing attraction strength, identification of two dynamical criteria for the non-clustered to clustered transition based on mean cluster lifetime and relaxation of local hexagonal order, pronounced non-Gaussian single-particle dynamics with an approximately exponential self-van Hove function in the equilibrium-cluster regime, and the preservation of anomalously enhanced large-scale collective diffusion under hydrodynamic interactions, with clustering causing an earlier onset of hydrodynamic effects compared to hard-sphere references.

Significance. If the simulation results hold, the work provides concrete evidence for the interplay between clustering, non-Gaussian diffusion, and hydrodynamic interactions in Q2D SALR systems, which are relevant to colloidal and soft-matter experiments. The direct comparison of LD and MPC simulations isolates the role of hydrodynamics in both single-particle and collective dynamics, and the reported earlier onset of HIs due to clustering offers a testable prediction for time-resolved scattering or microscopy studies.

major comments (1)
  1. [non-Gaussian dynamics / self-van Hove analysis] In the discussion of non-Gaussian dynamics, the statement that the approximately exponential self-van Hove function in the equilibrium-cluster phase is 'consistent with an underlying diffusing-diffusivity mechanism' is not accompanied by any direct test (e.g., extraction of short-time local diffusivities from trajectories and verification that their distribution or autocorrelation reproduces the observed van Hove tails). Without such a check, alternative sources of heterogeneity such as intermittent cluster trapping or caging cannot be ruled out, weakening the mechanistic attribution.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the constructive comment regarding the interpretation of non-Gaussian dynamics. We address it point by point below.

read point-by-point responses
  1. Referee: In the discussion of non-Gaussian dynamics, the statement that the approximately exponential self-van Hove function in the equilibrium-cluster phase is 'consistent with an underlying diffusing-diffusivity mechanism' is not accompanied by any direct test (e.g., extraction of short-time local diffusivities from trajectories and verification that their distribution or autocorrelation reproduces the observed van Hove tails). Without such a check, alternative sources of heterogeneity such as intermittent cluster trapping or caging cannot be ruled out, weakening the mechanistic attribution.

    Authors: We agree with the referee that the manuscript does not include a direct test of the diffusing-diffusivity mechanism via local diffusivity distributions or their autocorrelations. The original statement is limited to 'consistent with' based on the exponential shape matching a known signature in the literature, without claiming exclusivity. However, this does leave open alternative explanations such as intermittent trapping within clusters. We will revise the relevant paragraph to adopt more cautious language, explicitly note that other sources of heterogeneity cannot be ruled out, and suggest the proposed analysis as a possible extension. This addresses the concern without altering the reported observations. revision: yes

Circularity Check

0 steps flagged

No circularity: purely numerical simulation study with no derivations or fitted predictions.

full rationale

The manuscript reports results exclusively from Langevin dynamics (LD) and multiparticle collision dynamics (MPC) simulations of particle trajectories. No analytical derivations, self-referential equations, parameter fits renamed as predictions, or load-bearing self-citations appear in the provided text. Claims about non-Gaussian van Hove functions are presented as observations from the simulations and described only as 'consistent with' a mechanism, without any reduction to inputs by construction. The study is self-contained against external benchmarks via direct numerical output.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

As a simulation study, the work relies on standard numerical methods and interaction models from the field; no new free parameters or axioms are introduced beyond varying physical parameters like attraction strength and concentration.

pith-pipeline@v0.9.1-grok · 5833 in / 1167 out tokens · 43927 ms · 2026-06-26T10:58:45.789030+00:00 · methodology

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Works this paper leans on

111 extracted references

  1. [1]

    Liu and Y

    Y. Liu and Y. Xi, Curr. Opin. Colloid Interface Sci., 2019, 39, 123--136

  2. [2]

    Ruiz-Franco and E

    J. Ruiz-Franco and E. Zaccarelli, Annu. Rev. Condens. Matter Phys., 2021, 12, 51--70

  3. [3]

    Stradner, H

    A. Stradner, H. Sedgwick, F. Cardinaux, W. C. Poon, S. U. Egelhaaf and P. Schurtenberger, Nature, 2004, 432, 492--495

  4. [4]

    Z. Tan, V. Calandrini, J. K. G. Dhont and G. Nägele, Soft Matter, 2024, 20, 9528--9546

  5. [5]

    Destainville, M

    N. Destainville, M. Manghi and J. Cornet, Biomolecules, 2018, 8, 64

  6. [6]

    Wasnik, N

    V. Wasnik, N. S. Wingreen and R. Mukhopadhyay, PLoS One, 2015, 10, 1--13

  7. [7]

    J. J. Sieber, K. I. Willig, C. Kutzner, C. Gerding-Reimers, B. Harke, G. Donnert, B. Rammner, C. Eggeling, S. W. Hell, H. Grubmüller and T. Lang, Science, 2007, 317, 1072--1076

  8. [8]

    Gurry, O

    T. Gurry, O. Kahramanohgullari and R. G. Endres, PLoS One, 2009, 4, e6148

  9. [9]

    P. D. Godfrin, N. E. Valadez-Pérez, R. Castañeda-Priego, N. J. Wagner and Y. Liu, Soft Matter, 2014, 10, 5061--5071

  10. [10]

    Zhuang and P

    Y. Zhuang and P. Charbonneau, J. Phys. Chem. B, 2016, 120, 6178--6188

  11. [11]

    Zhuang and P

    Y. Zhuang and P. Charbonneau, J. Phys. Chem. B, 2016, 120, 7775--7782

  12. [12]

    Litniewski, W

    M. Litniewski, W. T. Gozdz and A. Ciach, Soft Matter, 2025, 21, 6801--6813

  13. [13]

    A. J. Archer, Phys. Rev. E, 2008, 78, 031402

  14. [14]

    Imperio and L

    A. Imperio and L. Reatto, J. Phys. Condens. Matter, 2004, 16, S3769

  15. [15]

    Imperio and L

    A. Imperio and L. Reatto, J. Chem. Phys., 2006, 124, 164712

  16. [16]

    Sciortino, S

    F. Sciortino, S. Mossa, E. Zaccarelli and P. Tartaglia, Phys. Rev. Lett., 2004, 93, 055701

  17. [17]

    A. I. Campbell, V. J. Anderson, J. S. van Duijneveldt and P. Bartlett, Phys. Rev. Lett., 2005, 94, 208301

  18. [18]

    C. L. Klix, C. P. Royall and H. Tanaka, Phys. Rev. Lett., 2010, 104, 165702

  19. [19]

    D. F. Schwanzer, D. Coslovich and G. Kahl, J. Phys. Condens. Matter, 2016, 28, 414015

  20. [20]

    Barhoum and A

    S. Barhoum and A. Yethiraj, J. Phys. Chem. B, 2010, 114, 17062--17067

  21. [21]

    Yearley, I

    E. Yearley, I. Zarraga, S. Shire, T. Scherer, Y. Gokarn, N. Wagner and Y. Liu, Biophys. J., 2013, 105, 720--731

  22. [22]

    P. D. Godfrin, S. D. Hudson, K. Hong, L. Porcar, P. Falus, N. J. Wagner and Y. Liu, Phys. Rev. Lett., 2015, 115, 228302

  23. [23]

    Yearley, P

    E. Yearley, P. Godfrin, T. Perevozchikova, H. Zhang, P. Falus, L. Porcar, M. Nagao, J. Curtis, P. Gawande, R. Taing, I. Zarraga, N. Wagner and Y. Liu, Biophys. J., 2014, 106, 1763--1770

  24. [24]

    P. D. Godfrin, I. E. Zarraga, J. Zarzar, L. Porcar, P. Falus, N. J. Wagner and Y. Liu, J. Phys. Chem. B, 2016, 120, 278--291

  25. [25]

    Porcar, P

    L. Porcar, P. Falus, W.-R. Chen, A. Faraone, E. Fratini, K. Hong, P. Baglioni and Y. Liu, J. Phys. Chem. Lett., 2010, 1, 126--129

  26. [26]

    Y. Liu, L. Porcar, J. Chen, W.-R. Chen, P. Falus, A. Faraone, E. Fratini, K. Hong and P. Baglioni, J. Phys. Chem. B, 2011, 115, 7238--7247

  27. [27]

    Nawrocki, P.-h

    G. Nawrocki, P.-h. Wang, I. Yu, Y. Sugita and M. Feig, J. Phys. Chem. B, 2017, 121, 11072--11084

  28. [28]

    S. Das, J. Riest, R. G. Winkler, G. Gompper, J. K. Dhont and G. N \"a gele, Soft Matter, 2018, 14, 92--103

  29. [29]

    P. D. Godfrin, P. Falus, L. Porcar, K. Hong, S. D. Hudson, N. J. Wagner and Y. Liu, Soft Matter, 2018, 14, 8570--8579

  30. [30]

    Perdomo-Pérez, J

    R. Perdomo-Pérez, J. Martínez-Rivera, N. C. Palmero-Cruz, M. A. Sandoval-Puentes, J. A. S. Gallegos, E. Lázaro-Lázaro, N. E. Valadez-Pérez, A. Torres-Carbajal and R. Castañeda-Priego, J. Phys. Condens. Matter, 2022, 34, 144005

  31. [31]

    M. K. Bera, B. Qiao, S. Seifert, B. P. Burton-Pye, M. Olvera de la Cruz and M. R. Antonio, J. Phys. Chem. C, 2016, 120, 1317--1327

  32. [32]

    Erlkamp, S

    M. Erlkamp, S. Grobelny, A. Faraone, C. Czeslik and R. Winter, J. Phys. Chem. B, 2014, 118, 3310--3316

  33. [33]

    Balbo, P

    J. Balbo, P. Mereghetti, D.-P. Herten and R. Wade, Biophys. J., 2013, 104, 1576--1584

  34. [34]

    Varga and J

    Z. Varga and J. Swan, Soft Matter, 2016, 12, 7670--7681

  35. [35]

    W. Kob, C. Donati, S. J. Plimpton, P. H. Poole and S. C. Glotzer, Phys. Rev. Lett., 1997, 79, 2827--2830

  36. [36]

    Reichhardt and C

    C. Reichhardt and C. J. Olson Reichhardt, Phys. Rev. Lett., 2003, 90, 095504

  37. [37]

    S. K. Schnyder, T. O. E. Skinner, A. L. Thorneywork, D. G. A. L. Aarts, J. Horbach and R. P. A. Dullens, Phys. Rev. E, 2017, 95, 032602

  38. [38]

    Kaur and S

    C. Kaur and S. P. Das, Phys. Rev. E, 2003, 67, 051505

  39. [39]

    C.-C. G. Yeh, H. W. Hatch, A. N. Sreenivasan, B. Bharti, V. K. Shen, Z. M. Sherman and T. M. Truskett, J. Phys. Chem. B, 2025, 129, 6428--6438

  40. [40]

    Hilger, M

    D. Hilger, M. Masureel and B. K. Kobilka, Nat. Struct. Mol. Biol., 2018, 25, 4--12

  41. [41]

    P. G. Saffman and M. Delbr \"u ck, Proc. Natl. Acad. Sci. U.S.A., 1975, 72, 3111--3113

  42. [42]

    Ramadurai, A

    S. Ramadurai, A. Holt, V. Krasnikov, G. van den Bogaart, J. A. Killian and B. Poolman, J. Am. Chem. Soc., 2009, 131, 12650--12656

  43. [43]

    J. Gao, Y. Shen, S. Komura, W. Hu, L. Shen and J. Hu, Proc. Natl. Acad. Sci. U.S.A., 2025, 122, e2503203122

  44. [44]

    Javanainen, H

    M. Javanainen, H. Martinez-Seara, R. Metzler and I. Vattulainen, J. Phys. Chem. Lett., 2017, 8, 4308--4313

  45. [45]

    Pesch\'e and G

    R. Pesch\'e and G. N\"agele, Phys. Rev. E, 2000, 62, 5432--5443

  46. [46]

    Pesché, M

    R. Pesché, M. Kollmann and G. Nägele, J. Chem. Phys., 2001, 114, 8701--8707

  47. [47]

    N \"a gele, A

    G. N \"a gele, A. J. Banchio, M. Kollmann and R. Pesch \'e , Mol. Phys., 2002, 100, 2921--2933

  48. [48]

    Bleibel, A

    J. Bleibel, A. Dom \' nguez and M. Oettel, Phys. Rev. E, 2017, 95, 032604

  49. [49]

    R. P. Pel \'a ez, F. B. Usabiaga, S. Panzuela, Q. Xiao, R. Delgado-Buscalioni and A. Donev, J. Stat. Mech., 2018, 2018, 063207

  50. [50]

    Panzuela and R

    S. Panzuela and R. Delgado-Buscalioni, Phys. Rev. Lett., 2018, 121, 048101

  51. [51]

    E. K. R. Mackay, S. Marbach, B. Sprinkle and A. L. Thorneywork, Phys. Rev. X, 2024, 14, 041016

  52. [52]

    Carter, E

    A. Carter, E. K. R. Mackay, B. Sprinkle, A. L. Thorneywork and S. Marbach, Soft Matter, 2025, 21, 3991--4002

  53. [53]

    Chamorro-Burgos and A

    M. Chamorro-Burgos and A. Dom\' nguez, Phys. Rev. E, 2026, 113, 055402

  54. [54]

    Panzuela, R

    S. Panzuela, R. P. Pel \'a ez and R. Delgado-Buscalioni, Phys. Rev. E, 2017, 95, 012602

  55. [55]

    Franosch, M

    T. Franosch, M. Grimm, M. Belushkin, F. M. Mor, G. Foffi, L. Forr \'o and S. Jeney, Nature, 2011, 478, 85--88

  56. [56]

    Belushkin, R

    M. Belushkin, R. Winkler and G. Foffi, J. Phys. Chem. B, 2011, 115, 14263--14268

  57. [57]

    Hansen and I

    J.-P. Hansen and I. R. McDonald, Theory of Simple Liquids (4th ed.), Academic Press, Oxford, 2013

  58. [58]

    A. J. C. Ladd, H. Gang, J. X. Zhu and D. A. Weitz, Phys. Rev. E, 1995, 52, 6550--6572

  59. [59]

    A. J. C. Ladd, H. Gang, J. X. Zhu and D. A. Weitz, Phys. Rev. Lett., 1995, 74, 318--321

  60. [60]

    Bakker and C

    A. Bakker and C. Lowe, J. Chem. Phys., 2002, 116, 5867--5876

  61. [61]

    Dom \' nguez, Phys

    A. Dom \' nguez, Phys. Rev. E, 2014, 90, 062314

  62. [62]

    Charbonneau and D

    P. Charbonneau and D. R. Reichman, Phys. Rev. E, 2007, 75, 050401

  63. [63]

    E. Mani, W. Lechner, W. K. Kegel and P. G. Bolhuis, Soft Matter, 2014, 10, 4479--4486

  64. [64]

    Sciortino, P

    F. Sciortino, P. Tartaglia and E. Zaccarelli, J. Phys. Chem. B, 2005, 109, 21942--21953

  65. [65]

    Zahn and G

    K. Zahn and G. Maret, Phys. Rev. Lett., 2000, 85, 3656--3659

  66. [66]

    Haghgooie and P

    R. Haghgooie and P. S. Doyle, Phys. Rev. E, 2005, 72, 011405

  67. [67]

    S. Z. Lin, B. Zheng and S. Trimper, Phys. Rev. E, 2006, 73, 066106

  68. [68]

    C. P. Kelleher, R. E. Guerra, A. D. Hollingsworth and P. M. Chaikin, Phys. Rev. E, 2017, 95, 022602

  69. [69]

    A. L. Thorneywork, J. L. Abbott, D. G. A. L. Aarts, P. Keim and R. P. A. Dullens, J. Phys. Condens. Matter, 2018, 30, 104003

  70. [70]

    B. I. Halperin and D. R. Nelson, Phys. Rev. Lett., 1978, 41, 121--124

  71. [71]

    D. R. Nelson and B. I. Halperin, Phys. Rev. B, 1979, 19, 2457--2484

  72. [72]

    Bialk\'e, T

    J. Bialk\'e, T. Speck and H. L\"owen, Phys. Rev. Lett., 2012, 108, 168301

  73. [73]

    Z\"ottl and H

    A. Z\"ottl and H. Stark, Phys. Rev. Lett., 2014, 112, 118101

  74. [74]

    Theers, E

    M. Theers, E. Westphal, K. Qi, R. G. Winkler and G. Gompper, Soft Matter, 2018, 14, 8590--8603

  75. [75]

    Pasupalak, L

    A. Pasupalak, L. Yan-Wei, R. Ni and M. Pica Ciamarra, Soft Matter, 2020, 16, 3914--3920

  76. [76]

    B. Wang, J. Kuo, S. C. Bae and S. Granick, Nat. Mater., 2012, 11, 481--485

  77. [77]

    Fuchs, W

    M. Fuchs, W. G\"otze and M. R. Mayr, Phys. Rev. E, 1998, 58, 3384--3399

  78. [78]

    Malevanets and R

    A. Malevanets and R. Kapral, J. Chem. Phys., 1999, 110, 8605--8613

  79. [79]

    Malevanets and R

    A. Malevanets and R. Kapral, J. Chem. Phys., 2000, 112, 7260--7269

  80. [80]

    Kapral, Adv

    R. Kapral, Adv. Chem. Phys., 2008, 140, 89--146

Showing first 80 references.