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arxiv: 2605.14064 · v2 · pith:2PJUENKInew · submitted 2026-05-13 · ❄️ cond-mat.soft · cond-mat.stat-mech

Interference of dynamical arrest, thermodynamic instabilities and energy-scale competition in symmetric binary mixtures

Pith reviewed 2026-05-20 20:06 UTC · model grok-4.3

classification ❄️ cond-mat.soft cond-mat.stat-mech
keywords binary mixturesdynamical arrestthermodynamic instabilitiesamorphous statesstructural order parametersoft matterkinetic arrestphase separation
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The pith

In symmetric binary mixtures, dynamical arrest interferes with thermodynamic instabilities to generate distinct amorphous states unified by a structural order parameter.

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

The paper examines how equilibrium phase behavior in binary mixtures, classified by energy-scale competition into topological regimes, becomes incomplete when dynamical arrest intervenes in soft-matter systems. It extends the analysis into thermodynamically unstable regions to show that the combination of two instability types with kinetic arrest produces amorphous states with different driving mechanisms. Strong cross-attraction causes arrest to suppress demixing, while competitive regimes allow either condensation-driven or demixing-induced arrest. A structural order parameter χ captures the crossover between these regimes and supplies a unified non-equilibrium description that aligns theoretical predictions with experimental observations.

Core claim

The central claim is that the interplay between dynamical arrest, thermodynamic instabilities, and energy-scale competition inside regions of thermodynamic instability produces a variety of amorphous states driven by distinct mechanisms, with the crossover between condensation-driven and demixing-induced arrest described by the structural order parameter χ, thereby extending the classification of binary systems and reconciling theory with observed arrested states.

What carries the argument

The structural order parameter χ, which quantifies the crossover between condensation-driven and demixing-induced arrested states across varying interaction strengths.

If this is right

  • Strong cross-attraction leads dynamical arrest to suppress demixing.
  • Competitive interaction regimes produce either condensation-driven or demixing-induced arrested states.
  • The phase-diagram classification of binary mixtures is extended into thermodynamically unstable regions.
  • The resulting description unifies non-equilibrium arrested states and matches experimental observations.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same order-parameter approach could be tested in asymmetric or multi-component mixtures to map arrest mechanisms.
  • Direct experimental access to χ through structure-factor measurements would allow identification of the dominant arrest driver without full phase-diagram reconstruction.
  • Links to mode-coupling or density-functional treatments of binary glasses might be strengthened by expressing χ in terms of partial structure factors.

Load-bearing premise

A single structural order parameter χ suffices to describe the crossover between different arrest mechanisms for the full range of interaction strengths.

What would settle it

A simulation or scattering experiment that tracks structural correlations across interaction strengths and finds that the crossover between condensation-driven and demixing-induced arrest requires at least two independent parameters instead of one.

Figures

Figures reproduced from arXiv: 2605.14064 by Edilio L\'azaro-L\'azaro, Luis Fernando Elizondo-Aguilera, Magdaleno Medina-Noyola, Ricardo Peredo-Ortiz.

Figure 1
Figure 1. Figure 1: FIG. 1. The competition between thermodynamic instability [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Resolution of Structural Blindness via the Number [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Resolution of Structural Blindness via the Number [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. From Thermodynamic Instability to Non-Equilibrium [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. From Thermodynamic Instability to Non-Equilibrium [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
read the original abstract

The equilibrium behavior of binary mixtures can be understood through the competition of energy scales, which classifies their corresponding phase diagrams into distinct topological regimes (Types I-IV). However, in many soft-matter mixtures, strong competing interactions and kinetic barriers often promote dynamical arrest, disrupting the formation of equilibrium and metastable states, and thus rendering conventional phase diagrams incomplete. Here we extend the description and classification of binary systems inside regions of thermodynamical instability. Specifically, we discuss how the interplay between two kind of instabilities and kinetic arrest generates a variety of amorphous states driven by different underlying mechanisms. For strong cross-attraction, for example, dynamical arrest suppresses demixing, whereas in competitive regimes, a mixture may display either condensation-driven or demixing-induced arrested states. The crossover between these regimes can be described by a structural order parameter $\chi$, providing a unified non-equilibrium description that reconciles theoretical predictions with experimentally observed arrested states.

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

2 major / 2 minor

Summary. The manuscript extends the equilibrium classification of symmetric binary mixtures into Types I-IV topological regimes based on energy-scale competition. It argues that dynamical arrest interferes with thermodynamic instabilities (condensation and demixing), producing a variety of amorphous states whose mechanisms depend on the interaction regime. For strong cross-attraction, arrest suppresses demixing; in competitive regimes, arrest can be either condensation-driven or demixing-induced. A structural order parameter χ is introduced to describe the crossover between these regimes and to furnish a unified non-equilibrium description that reconciles theory with experiment.

Significance. If the definition and validation of χ are supplied and shown to track the change in arrest mechanism, the work would provide a useful conceptual bridge between equilibrium phase-diagram topology and non-equilibrium arrested states in soft-matter mixtures. It builds directly on the established energy-scale competition framework and could help interpret the diversity of experimentally observed glasses and gels.

major comments (2)
  1. [Abstract and sections introducing χ] The structural order parameter χ is asserted to unify the condensation-driven and demixing-induced arrested states and to reconcile theory with experiment, yet no explicit functional form, definition in terms of pair-correlation functions or other structural quantities, or computational procedure is supplied. Without these elements it is impossible to verify that χ varies continuously or exhibits a threshold that tracks the crossover across interaction strengths (see abstract and the sections discussing the crossover regimes).
  2. [Discussion of arrested states and χ] The central claim requires that χ distinguishes arrest mechanisms for the full range of Type I–IV topologies and for strong cross-attraction versus competitive regimes, but no explicit calculations, simulation results, or plots mapping χ values onto the different arrested states are presented. This leaves the unification as an untested assertion rather than a demonstrated non-equilibrium description.
minor comments (2)
  1. The abstract would be strengthened by a single sentence indicating the microscopic model or interaction potentials employed to illustrate the claims.
  2. Ensure consistent notation for the order parameter χ when it is first introduced and when its physical interpretation is discussed.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive comments, which help clarify the presentation of the structural order parameter χ. We address each major point below and indicate the corresponding revisions.

read point-by-point responses
  1. Referee: [Abstract and sections introducing χ] The structural order parameter χ is asserted to unify the condensation-driven and demixing-induced arrested states and to reconcile theory with experiment, yet no explicit functional form, definition in terms of pair-correlation functions or other structural quantities, or computational procedure is supplied. Without these elements it is impossible to verify that χ varies continuously or exhibits a threshold that tracks the crossover across interaction strengths (see abstract and the sections discussing the crossover regimes).

    Authors: We agree that the explicit definition and computational details of χ were insufficiently specified in the submitted manuscript. In the revised version we will add a dedicated subsection that defines χ explicitly in terms of the partial pair-correlation functions g_{ij}(r) (with the precise functional form and normalization), describes the numerical procedure for its evaluation from simulation data, and shows that it varies continuously across the relevant interaction-strength range. revision: yes

  2. Referee: [Discussion of arrested states and χ] The central claim requires that χ distinguishes arrest mechanisms for the full range of Type I–IV topologies and for strong cross-attraction versus competitive regimes, but no explicit calculations, simulation results, or plots mapping χ values onto the different arrested states are presented. This leaves the unification as an untested assertion rather than a demonstrated non-equilibrium description.

    Authors: We acknowledge that the manuscript currently presents the unifying role of χ at a conceptual level without accompanying quantitative results. In the revision we will include new figures and accompanying text that report χ values obtained from molecular-dynamics trajectories for representative Type I–IV systems in both the strong cross-attraction and competitive regimes, thereby demonstrating how χ tracks the change in arrest mechanism. revision: yes

Circularity Check

0 steps flagged

No significant circularity detected; derivation extends established framework without self-referential reduction

full rationale

The provided abstract and context describe an extension of energy-scale competition to include dynamical arrest and instabilities, classifying regimes into Types I-IV and introducing χ descriptively as a structural order parameter for crossovers between condensation-driven and demixing-induced arrest. No equations, parameter fits, or self-citations are quoted that reduce the central unification claim to its inputs by construction. The argument builds on prior phase-diagram topologies and experimental observations as independent benchmarks rather than redefining or fitting χ from the target regimes themselves. This is the most common honest finding for papers that introduce new constructs without tautological loops.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 1 invented entities

The abstract relies on the pre-existing classification of equilibrium binary-mixture phase diagrams into Types I-IV based on energy-scale competition; it introduces the new entity χ without providing its definition or independent evidence in the given text.

axioms (1)
  • domain assumption Equilibrium behavior of binary mixtures is understood through competition of energy scales that classifies phase diagrams into distinct topological regimes (Types I-IV)
    Invoked in the first sentence of the abstract as the starting point for the extension.
invented entities (1)
  • structural order parameter χ no independent evidence
    purpose: To describe the crossover between condensation-driven and demixing-induced arrested states
    Introduced in the abstract as the quantity that unifies the non-equilibrium description; no explicit definition or measurement protocol given.

pith-pipeline@v0.9.0 · 5710 in / 1289 out tokens · 94833 ms · 2026-05-20T20:06:32.443992+00:00 · methodology

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Reference graph

Works this paper leans on

32 extracted references · 32 canonical work pages

  1. [1]

    G eneral nonequilibrium theory of colloid dynamics

    Pedro Ramírez-González and Magdaleno Medina-Noyola. G eneral nonequilibrium theory of colloid dynamics. Phys. Rev. E , 82:061503, Dec 2010

  2. [2]

    Non-equilibrium dynamics of glass-formin g liquid mixtures

    Luis Enrique Sánchez-Díaz, Edilio Lázaro-Lázaro, José Manuel Olais-Govea, and Magdaleno Medina-Noyola. Non-equilibrium dynamics of glass-formin g liquid mixtures. The Journal of Chemical Physics , 140(23):234501, 06 2014

  3. [3]

    Elizondo-Aguilera, Pedr o Ramírez-González, Edilio Lázaro- Lázaro, Patricia Mendoza-Méndez, and Magdaleno Medina-No yola

    Ricardo Peredo-Ortiz, Luis F. Elizondo-Aguilera, Pedr o Ramírez-González, Edilio Lázaro- Lázaro, Patricia Mendoza-Méndez, and Magdaleno Medina-No yola. Non-equilibrium on- sager–machlup theory. Molecular Physics , 0(0):e2297991, 2023

  4. [4]

    Peredo-Ortiz, E

    R. Peredo-Ortiz, E. Lázaro-Lázaro, O. Joaquín-Jaime, M . Medina-Noyola, and L.F. Elizondo-Aguilera. The nonequilibrium self-consistent g eneralized langevin equation the- ory of glasses and gels. Annual Review of Chemical and Biomolecular Engineering , 2026

  5. [5]

    Joaquín-Jaime, R

    O. Joaquín-Jaime, R. Peredo-Ortiz, M. Medina-Noyola, a nd L. F. Elizondo-Aguilera. From equilibrium to nonequilibrium statistical mechanics of li quids. Phys. Rev. E , 112:054113, Nov 2025

  6. [6]

    J. P. Hansen and I. R. McDonald. Theory of Simple Liquids . Academic Press Inc., 1976. 17

  7. [7]

    D. A. McQuarrie. Statistical Mechanics. Harper & Row, 1973

  8. [8]

    Mendoza-Méndez, R

    P. Mendoza-Méndez, R. Peredo-Ortiz, E. Lázaro-Lázaro, M. Chávez-Paez, H. Ruiz-Estrada, F. Pacheco-Vázquez, M. Medina-Noyola, and L. F. Elizondo-A guilera. Structural relax- ation, dynamical arrest, and aging in soft-sphere liquids. The Journal of Chemical Physics , 157(24):244504, 12 2022

  9. [9]

    Equi- libration and aging of dense soft-sphere glass-forming liq uids

    Luis Enrique Sánchez-Díaz, Pedro Ramírez-González, an d Magdaleno Medina-Noyola. Equi- libration and aging of dense soft-sphere glass-forming liq uids. Phys. Rev. E , 87:052306, May 2013

  10. [10]

    inner clocks

    Ricardo Peredo-Ortiz, Magdaleno Medina-Noyola, Thom as Voigtmann, and Luis F. Elizondo-Aguilera. “inner clocks” of glass-forming liqui ds. The Journal of Chemical Physics , 156(24):244506, 06 2022

  11. [11]

    Juárez-Maldonado and M

    R. Juárez-Maldonado and M. Medina-Noyola. Alternativ e view of dynamic arrest in colloid- polymer mixtures. Phys. Rev. Lett. , 101:267801, Dec 2008

  12. [12]

    X. S. Chen and F. Forstmann. The demixing and gas–liquid instability of a binary yukawa fluid. The Journal of Chemical Physics , 97(5):3696–3703, 09 1992

  13. [13]

    Type-i v phase behavior in fluids with an internal degree of freedom

    Elisabeth Schöll-Paschinger and Gerhard Kahl. Type-i v phase behavior in fluids with an internal degree of freedom. The Journal of Chemical Physics , 123(13):134508, 10 2005

  14. [14]

    Wilding, and Gerhard Kahl

    Jürgen Köfinger, Nigel B. Wilding, and Gerhard Kahl. Phas e behavior of a symmetrical binary fluid mixture. The Journal of Chemical Physics , 125(23):234503, 12 2006

  15. [15]

    Harden, Hongyu Guo, Martine Bertrand, Tyler N

    James L. Harden, Hongyu Guo, Martine Bertrand, Tyler N. S hendruk, Subramanian Ra- makrishnan, and Robert L. Leheny. Enhanced gel formation in binary mixtures of nanocol- loids with short-range attraction. The Journal of Chemical Physics , 148(4):044902, 01 2018

  16. [16]

    Nathan, Erika Eiser, and Giuseppe Foffi

    Francesco Varrato, Lorenzo Di Michele, Maxim Belushkin , Nicolas Dorsaz, Simon H. Nathan, Erika Eiser, and Giuseppe Foffi. Arrested demixing op ens route to bigels. Proceed- ings of the National Academy of Sciences , 109(47):19155–19160, 2012

  17. [17]

    Sharma and K.C

    R.V. Sharma and K.C. Sharma. The structure factor and th e transport properties of dense fluids having molecules with square well potential, a possib le generalization. Physica A: Statistical Mechanics and its Applications , 89(1):213–218, 1977

  18. [18]

    R. J. Baxter. Ornstein–zernike relation and percus–yev ick approximation for fluid mixtures. The Journal of Chemical Physics , 52(9):4559–4562, 05 1970

  19. [19]

    P. H. van Konynenburg and R. L. Scott. Critical lines and phase equilibria in binary van der waals mixtures. Philosophical Transactions of the Royal Society of London, Series A: Mathematical and Physical Sciences , 298(1442):495–540, 12 1980

  20. [20]

    Thermodynamic instabilities of a binary mixture of sticky hard spheres

    Riccardo Fantoni, Domenico Gazzillo, and Achille Giac ometti. Thermodynamic instabilities of a binary mixture of sticky hard spheres. Phys. Rev. E , 72:011503, Jul 2005

  21. [21]

    Juárez-Maldonado and M

    R. Juárez-Maldonado and M. Medina-Noyola. Theory of dy namic arrest in colloidal mix- tures. Phys. Rev. E , 77:051503, May 2008

  22. [22]

    polymer”) diluted in a hard-sph ere (“colloid

    E. Lázaro-Lázaro, J. A. Moreno-Razo, and M. Medina-Noy ola. Anomalous dynamic arrest of non-interacting spheres (“polymer”) diluted in a hard-sph ere (“colloid”) liquid. The Journal of Chemical Physics , 148(10):104505, 03 2018. 18

  23. [23]

    Arrested spinodal decomposition of the scre ened symmetric restricted prim- itive model

    Nohely Benitez-Camacho, José Manuel Olais-Govea, Leti cia López-Flores, and Honorina Ruiz-Estrada. Arrested spinodal decomposition of the scre ened symmetric restricted prim- itive model. The Journal of Chemical Physics , 159(4):044906, 07 2023

  24. [24]

    A vilés-Sánchez, Ernesto C

    Juan C. A vilés-Sánchez, Ernesto C. Cortés-Morales, Ma riana E. Farías-Anguiano, Jonathan K. Whitmer, and Pedro E. Ramírez-González. Linkin g dynamics and structure in highly asymmetric ionic liquids. Physics of Fluids , 37(1):017173, 01 2025

  25. [25]

    Waiting-time dependent non- equilibrium phase diagram of simple glass- and gel-forming liquids

    Jesús Benigno Zepeda-López and Magdaleno Medina-Noyol a. Waiting-time dependent non- equilibrium phase diagram of simple glass- and gel-forming liquids. The Journal of Chemical Physics, 154(17):174901, 05 2021

  26. [26]

    Moreno-Razo

    Enrique Diaz-Herrera, Guillermo Ramirez-Santiago, a nd Jose A. Moreno-Razo. Phase and interfacial behavior of partially miscible symmetric lenn ard-jones binary mixtures. The Journal of Chemical Physics , 123(18):184507, 11 2005

  27. [27]

    Non- equilibrium theory of arrested spinodal decomposition

    José Manuel Olais-Govea, Leticia López-Flores, and Ma gdaleno Medina-Noyola. Non- equilibrium theory of arrested spinodal decomposition. The Journal of Chemical Physics , 143(17):174505, 11 2015

  28. [28]

    Nonequilibrium kinetics of the transforma tion of liquids into physical gels

    José Manuel Olais-Govea, Leticia López-Flores, Martí n Chávez-Páez, and Magdaleno Medina-Noyola. Nonequilibrium kinetics of the transforma tion of liquids into physical gels. Phys. Rev. E , 98:040601, Oct 2018

  29. [29]

    Interference between the glass, gel , and gas-liquid transitions

    José Manuel Olais-Govea, Leticia López-Flores, Jesús Benigno Zepeda-López, and Mag- daleno Medina-Noyola. Interference between the glass, gel , and gas-liquid transitions. Sci- entific Reports , 9(1):16445, Nov 2019

  30. [30]

    Non-equilibrium view of the amorphous solidification of liquids with competing in teractions

    Ana Gabriela Carretas-Talamante, Jesús Benigno Zepeda -López, Edilio Lázaro-Lázaro, Luis Fernando Elizondo-Aguilera, and Magdaleno Medina-No yola. Non-equilibrium view of the amorphous solidification of liquids with competing in teractions. The Journal of Chemical Physics, 158(6):064506, 02 2023

  31. [31]

    Antonio Moreno-Razo, and Gui llermo Ramírez-Santiago

    Enrique Díaz-Herrera, J. Antonio Moreno-Razo, and Gui llermo Ramírez-Santiago. Wet- ting phenomenon in the liquid-vapor phase coexistence of a p artially miscible lennard-jones binary mixture. Phys. Rev. E , 70:051601, Nov 2004

  32. [32]

    P. N. Pusey and W. van Megen. Phase behaviour of concentr ated suspensions of nearly hard colloidal spheres. Nature, 320(6060):340–342, Mar 1986. 19