Pith. sign in

REVIEW 1 major objections 1 minor 63 references

A model of supercooled water links its liquid-liquid critical point to inversion thermodynamics of gas throttling.

Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →

T0 review · grok-4.3

2026-06-30 14:35 UTC pith:VI642PJG

load-bearing objection New model reproduces the Speedy-Angell and Poole pictures but the claimed analogy to Joule-Thomson inversion and black holes supplies no shown structural link that would add independent plausibility to the LLCP. the 1 major comments →

arxiv 2605.24105 v1 pith:VI642PJG submitted 2026-05-22 cond-mat.stat-mech

Theory of supercooled water

classification cond-mat.stat-mech
keywords supercooled waterliquid-liquid critical pointJoule-Thomson inversionmetastable liquidsthermodynamic analogystability limit
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved

The pith

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

The paper introduces a thermodynamic model for water that includes true supercooled liquid states metastable with respect to ice. Numerical solutions of the model recover both the stability-limit picture of Speedy and Angell and the metastable liquid-liquid critical point picture of Poole and colleagues. The authors identify an unnoticed analogy between the liquid-liquid critical point and the inversion curve in the Joule-Thomson throttling process for gases, with an extension to equivalent black hole phenomenology. This analogy is presented as lending significant theoretical plausibility to the actual existence of the liquid-liquid critical point in water.

Core claim

Numerical solutions of a model contemplating metastable supercooled-liquid states reproduce the Speedy-Angell stability-limit picture and Poole et al.'s liquid-liquid criticality, with the real existence of the liquid-liquid critical point gaining significant theoretical plausibility from a hitherto unnoticed analogy with the inversion thermodynamics of the Joule-Thomson gas throttling process and equivalent black hole phenomenology.

What carries the argument

The analogy between water's liquid-liquid critical point and the inversion curve of the Joule-Thomson gas throttling process, which maps thermodynamic inversion behavior across systems.

Load-bearing premise

The model assumes true supercooled-liquid states that are metastable with respect to crystalline solids and that its numerical solutions faithfully reproduce the Speedy-Angell and Poole pictures.

What would settle it

A calculation or measurement showing that thermodynamic properties near any liquid-liquid critical point in supercooled water fail to match the inversion curve signatures of the Joule-Thomson process would remove the analogy's support for the critical point's existence.

Watch this falsifier — get emailed when new claim-graph text bears on it.

If this is right

  • The liquid-liquid critical point, if present, should exhibit inversion-like thermodynamic responses similar to those in gas throttling.
  • The stability-limit and liquid-liquid critical point descriptions of supercooled water can be recovered within a single model framework.
  • The same inversion analogy extends the critical point phenomenology to black hole systems.

Where Pith is reading between the lines

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

  • The analogy might permit estimating the critical point coordinates in water from known inversion data on gases.
  • The approach could generalize to other liquids showing density or compressibility anomalies.
  • Experimental searches for the critical point could target regions where inversion thermodynamics predicts specific heat capacity or expansivity behaviors.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit.

Referee Report

1 major / 1 minor

Summary. The manuscript introduces a model of water that contemplates true supercooled-liquid states metastable with respect to the crystalline-solid ones. Its numerical solutions reproduce the Speedy-Angell stability-limit picture and Poole et al.'s metastable liquid-liquid criticality. The real existence of a liquid-liquid critical point is argued to gain significant theoretical plausibility from a hitherto unnoticed analogy with the inversion thermodynamics of the Joule-Thomson gas throttling process and, by extension, with equivalent phenomenology in black holes.

Significance. If the analogy is shown to rest on a rigorous structural mapping (rather than qualitative resemblance) that independently supports the LLCP, the work could strengthen the theoretical case for liquid-liquid criticality in supercooled water by linking it to established thermodynamic features of gases and gravitational systems. The reproduction of the Speedy-Angell and Poole pictures is a positive feature, but the central novelty claim depends on the analogy's independence from the model's fitted behavior.

major comments (1)
  1. [Abstract] Abstract: The claim that the LLCP 'gains significant theoretical plausibility' from the analogy with Joule-Thomson inversion thermodynamics is not accompanied by evidence of a structural mapping. No indication is given that the model's equation of state or free-energy functional possesses an inversion curve (or equivalent extremum) whose existence is mathematically tied to the LLCP in the same way the JT inversion curve is tied to the van der Waals critical point. Without this derivation, the analogy remains qualitative and does not confer independent plausibility on the central claim.
minor comments (1)
  1. The abstract refers to 'numerical solutions' reproducing known pictures but provides no information on the model's functional form, free parameters, or validation against simulation data; the main text should include these details for reproducibility.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading and constructive feedback on our manuscript. We address the single major comment below, indicating planned revisions where appropriate.

read point-by-point responses
  1. Referee: [Abstract] Abstract: The claim that the LLCP 'gains significant theoretical plausibility' from the analogy with Joule-Thomson inversion thermodynamics is not accompanied by evidence of a structural mapping. No indication is given that the model's equation of state or free-energy functional possesses an inversion curve (or equivalent extremum) whose existence is mathematically tied to the LLCP in the same way the JT inversion curve is tied to the van der Waals critical point. Without this derivation, the analogy remains qualitative and does not confer independent plausibility on the central claim.

    Authors: We agree with the referee that the manuscript presents the analogy with Joule-Thomson inversion thermodynamics (and black-hole phenomenology) as a qualitative parallel without deriving a rigorous structural mapping or demonstrating that the model's free-energy functional possesses an inversion curve mathematically linked to the LLCP in the same manner as for the van der Waals gas. The analogy is noticed and discussed as an interesting thermodynamic resemblance, but it does not rest on an independent mathematical equivalence that would confer additional plausibility beyond the model's own solutions. We will therefore revise the abstract to remove the phrasing that the LLCP 'gains significant theoretical plausibility' from the analogy and will instead describe the parallel as a noteworthy qualitative connection that may warrant further investigation. A clarifying sentence will also be added in the main text. This is a partial revision: we retain the observation of the analogy but temper the claim regarding its implications. revision: partial

Circularity Check

0 steps flagged

No significant circularity; central claim rests on presented analogy without reduction to inputs.

full rationale

The paper introduces a model of supercooled water whose numerical solutions are stated to reproduce the Speedy-Angell stability-limit picture and Poole et al. liquid-liquid criticality. The load-bearing claim for real existence of the LLCP is an analogy to Joule-Thomson inversion thermodynamics and black-hole phenomenology, described as 'hitherto unnoticed.' No equations, self-citations, fitted parameters renamed as predictions, or ansatzes smuggled via prior work are quoted in the provided text. The derivation chain does not reduce any prediction to its own inputs by construction; the analogy supplies independent content whose structural mapping is asserted rather than shown to be tautological. This is the normal case of a self-contained model plus external analogy.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 1 invented entities

Abstract-only review; no specific free parameters, axioms, or invented entities can be extracted beyond the model itself being postulated to allow metastable supercooled states.

invented entities (1)
  • The model of water no independent evidence
    purpose: To contemplate true supercooled-liquid states metastable with respect to crystalline solids
    Introduced to enable numerical reproduction of stability-limit and liquid-liquid criticality pictures.

pith-pipeline@v0.9.1-grok · 5609 in / 1197 out tokens · 41282 ms · 2026-06-30T14:35:49.804410+00:00 · methodology

0 comments
read the original abstract

We introduce a model of water contemplating true supercooled-liquid states that, as such, are metastable with respect to the crystalline-solid ones. Its numerical solutions reproduce from Speedy-Angell's stability-limit picture to Poole et al.'s metastable liquid--liquid criticality. The real existence of a liquid--liquid critical point is found to gain significant theoretical plausibility from a hitherto unnoticed analogy with the ``inversion thermodynamics'' of Joule-Thomson gas throttling process and, by extension, with the equivalent phenomenology exhibited by black holes.

Figures

Figures reproduced from arXiv: 2605.24105 by Claudio A. Cerdeiri\~na, Jacobo Troncoso.

Figure 1
Figure 1. Figure 1: FIG. 1: Two-dimensional illustration of individual cell states [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: Numerical results for our five-state model with parameter setting “1.” (Left) Pressure [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: Numerical results for our five-state model with pa [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Its upper left panel illustrates water’s unusual [PITH_FULL_IMAGE:figures/full_fig_p003_4.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: (Left) Molecular simulation results for the [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

63 extracted references · 63 canonical work pages

  1. [1]

    critical-point-free scenario

    The supercooled liquid spinodal is now absent. It is superseded by a binodal corresponding to coexistence between HDL and LDL phases and terminating at a sec- ondcpoint. This is the second-critical-point scenario put forth by Poole et al. [10]. The whole transition is metastable with respect to the crystalline solid phase, which certainly corresponds to t...

  2. [2]

    This implies that the locus of temperatures of maximum density TMD is also that of temperatures of minimum volume per par- ticle

    Note that av(T) minimum corresponds to aρ(T) maxi- mum, withρ≡v −1 the number density. This implies that the locus of temperatures of maximum density TMD is also that of temperatures of minimum volume per par- ticle. We use throughout the paper the acronym TMD since it is the most popular one

  3. [3]

    R. J. Speedy and C. A. Angell, Isothermal compressibility of supercooled water and evidence for a thermodynamic singularity at –45 C, J. Chem. Phys.65, 851 (1976)

  4. [4]

    C. A. Angell, M. Oguni, and W. J. Sichina, Heat capacity of water at extremes of supercooling and superheating, J. Phys. Chem.86, 998 (1982)

  5. [5]

    D. E. Hare and C. M. Sorensen, The density of super- cooled water. 2. Bulk samples cooled to the homogeneous nucleation limit, J. Chem. Phys.87, 4840 (1987)

  6. [6]

    Holten, C

    V. Holten, C. Qiu, E. Guillerm, M. Wilke, J. Ricka, 5 M. Frenz, and F. Caupin, Compressibility anomalies in stretched water and their interplay with density anoma- lies, J. Phys. Chem. Lett.8, 5519 (2017)

  7. [7]

    K. H. Kim et al., Maxima in the thermodynamic response and correlation functions of deeply supercooled water, Science358, 1589 (2017)

  8. [8]

    Pathak et al., Enhancement and maximum in the iso- baric specific-heat capacity measurements of deeply su- percooled water using ultrafast calorimetry, Proc

    H. Pathak et al., Enhancement and maximum in the iso- baric specific-heat capacity measurements of deeply su- percooled water using ultrafast calorimetry, Proc. Natl. Acad. Sci. U. S. A.118, e2018379118 (2021)

  9. [9]

    R. J. Speedy, Stability-limit conjecture. An interpreta- tion of the properties of water, J. Phys. Chem.86, 982 (1982)

  10. [10]

    Chitnelawong, F

    P. Chitnelawong, F. Sciortino, and P. H. Poole, The stability-limit conjecture revisited, J. Chem. Phys.150, 234502 (2019)

  11. [11]

    P. H. Poole, F. Sciortino, U. Essmann, and H. E. Stanley, Phase behavior of metastable water, Nature360, 324 (1992)

  12. [12]

    J. C. Palmer, F. Martelli, Y. Liu, R. Car, A. Z. Pana- giotopoulos, and P. G. Debenedetti, Metastable liquid- liquid transition in a molecular model of water, Nature 510, 385 (2014)

  13. [13]

    J. C. Palmer, P. H. Poole, F. Sciortino, and P. G. Debenedetti, Advances in computational studies of the liquid–liquid transition in water and water-like models, Chem. Rev.118, 9129 (2018)

  14. [14]

    P. G. Debenedetti, F. Sciortino, and G. Zerze, Second critical point in two realistic models of water, Science 369, 289 (2020)

  15. [15]

    J. Weis, F. Sciortino, A. Z. Panagiotopoulos, and P. G. Debenedetti, Liquid–liquid criticality in the WAIL water model, J. Chem. Phys.157, 024502 (2022)

  16. [16]

    T. E. Gartner, P. M. Piaggi, R. Car, A. Z. Panagiotopou- los, and P. G. Debenedetti, Liquid–liquid transition in water from first principles, Phys. Rev. Lett.129, 255702 (2022)

  17. [17]

    Sciortino, Y

    F. Sciortino, Y. Zhai, S. L. Bore, and F. Paesani, Con- straints on the location of the liquid–liquid critical point in water, Nat. Phys.21, 480 (2025)

  18. [18]

    Sastry, P

    S. Sastry, P. G. Debenedetti, F. Sciortino, and H. E. Stanley, Singularity-free interpretation of the thermo- dynamics of supercooled water, Phys. Rev. E53, 6144 (1996)

  19. [19]

    L. P. N. Rebelo, P. G. Debenedetti, and S. Sastry, Singularity-free interpretation of the thermodynamics of supercooled water. II. Thermal and volumetric behavior, J. Chem. Phys.106, 626 (1998)

  20. [20]

    Kringle, W

    L. Kringle, W. A. Thornley, B. D. Kay, and G. A. Kim- mel, Reversible structural transformations in supercooled liquid water from 135 to 245 K, Science369, 1490 (2020)

  21. [21]

    K. H. Kim et al., Experimental observation of the liquid– liquid transition in bulk supercooled water under pres- sure, Science370, 978 (2020)

  22. [22]

    Amann-Winkel et al., Liquid–liquid phase separa- tion in supercooled water from ultrafast heating of low- density amorphous ice, Nature Comm.14, 442 (2023)

    K. Amann-Winkel et al., Liquid–liquid phase separa- tion in supercooled water from ultrafast heating of low- density amorphous ice, Nature Comm.14, 442 (2023)

  23. [23]

    You et al., Experimental evidence of a liquid–liquid critical point in supercooled water, Science391, 1387 (2026)

    S. You et al., Experimental evidence of a liquid–liquid critical point in supercooled water, Science391, 1387 (2026)

  24. [24]

    P. H. Poole, F. Sciortino, T. Grande, H. E. Stanley, and C. A. Angell, Effect of hydrogen bonds on the thermo- dynamic behavior of liquid water, Phys. Rev. Lett.73, 1632 (1994)

  25. [25]

    T. M. Truskett, P. G. Debenedetti, S. Sastry, and S. Torquato, A single-bond approach to orientation- dependent interactions and its implications for liquid wa- ter, J. Chem. Phys.111, 2647 (1999)

  26. [26]

    T. M. Truskett and K. A. Dill, A simple statistical me- chanical model of water, J. Phys. Chem. B106, 11829 (2002)

  27. [27]

    Franzese and H

    G. Franzese and H. E. Stanley, Liquid-liquid critical point in a hamiltonian model for water: analytic solution, J. Phys.: Condens Matter14, 2201 (2002)

  28. [28]

    Ciach, W

    A. Ciach, W. Gozdz, and A. Perera, Simple three-state lattice model for liquid water, Phys. Rev E78, 021203 (2008)

  29. [29]

    Stokely, M

    K. Stokely, M. C. Mazza, H. E. Stanley, and G. Franzese, Effect of hydrogen bond cooperativity on the behavior of water, Proc. Natl. Acad. Sci. U. S. A.107, 1301 (2010)

  30. [30]

    C. A. Cerdeiri˜ na and H. E. Stanley, Ising-like models with energy-volume coupling, Phys. Rev. Lett.120, 120603 (2018)

  31. [31]

    Urbic and K

    T. Urbic and K. A. Dill, Water is a cagey liquid, J. Am. Chem. Soc.140, 17106 (2018)

  32. [32]

    C. A. Cerdeiri˜ na, J. Troncoso, D. Gonz´ alez-Salgado, P. G. Debenedetti, and H. E. Stanley, Water’s two-critical- point scenario in the Ising paradigm, J. Chem. Phys.150, 244509 (2019)

  33. [33]

    Caupin and M

    F. Caupin and M. A. Anisimov, Minimal microscopic model for liquid polyamorphism and waterlike anoma- lies, Phys. Rev. Lett.127, 185701 (2021)

  34. [34]

    L. E. Coronas and G. Franzese, Phase behavior of metastable water from large-scale simulations of a quan- titatively accurate model near ambient conditions: The liquid-liquid critical point, J. Chem. Phys.161, 164502 (2024)

  35. [35]

    C. A. Cerdeiri˜ na and J. Troncoso, Ising paradigm in iso- baric ensembles, Entropy26, 438 (2024)

  36. [36]

    Verma and K

    L. Verma and K. A. Dill, Statistical mechanical theory of liquid water, J. Chem. Theory Comp.21, 7755 (2025)

  37. [37]

    Troncoso and C

    J. Troncoso and C. A. Cerdeiri˜ na, Ising model for the freezing transition, Phys. Rev. E109, 014123 (2024)

  38. [38]

    Troncoso and C

    J. Troncoso and C. A. Cerdeiri˜ na, Mean-field theory for the metastable states of a simple substance, Phys. Rev. E112, 014103 (2025)

  39. [39]

    Ising model

    The term “Ising model” defectively refers to the most elementary versions with two states for individual lat- tice sites, but it also comprises in a broader sense more elaborated versions with an arbitrary number of states. Nomenclature using quantum-mechanical language is “spin-S” models, whereS= 1 2 for two states,S= 1 for three,S= 3 2 for four, etc. Mo...

  40. [40]

    Penrose and J

    Mean-field theory contemplates metastable states as 6 truly thermodynamic states: see, e.g., O. Penrose and J. L. Lebowitz, Rigorous treatment of metastable states in the van der Waals-Maxwell theory, J. Stat. Phys.3, 211 (1971). For systems composed by particles interact- ing via short-range forces, mean-field theory is only exact for the abstract case o...

  41. [41]

    S. J. Hawking and D. N. Page, Thermodynamics of black holes in anti-de Sitter space, Comm. Math. Phys.87, 577 (1983)

  42. [42]

    Chamblin, R

    A. Chamblin, R. Emparan, C. V. Johnson, and R. C. Myers, Charged AdS black holes and catastrophic holog- raphy, Phys. Rev. D60, 064018 (1999)

  43. [43]

    Kastor, S

    D. Kastor, S. Ray, and J. Traschen, Enthalpy and the mechanics of AdS black holes, Class. Quantum Grav.26, 195011 (2009)

  44. [44]

    B. P. Dolan, Pressure and volume in the first law of black hole thermodynamics, J. High Energy Phys.28, 235017 (2011)

  45. [45]

    Kubiznak and R

    D. Kubiznak and R. B. Mann, P-V criticality of charged AdS black holes, J. High Energy Phys.2012, 33 (2012)

  46. [46]

    ¨Okc¨ u and E

    O. ¨Okc¨ u and E. Aydmer, Joule–Thomson expansion of the charged AdS black holes, Eur. Phys. J. C77, 24 (2017)

  47. [47]

    No account for the plethora of ice phases is provided. Taking into account that underlying them is a number of distinct crystalline lattices, one should not realistically expect to characterize the full range of ice polymorphs from a mean-field calculation that, as such, is insensitive to lattice structure. In any event, a crude description of ice phases ...

  48. [48]

    The notion of fluctuating cell volumes and free volumes in Ising-like models is relatively recent: C. A. Cerdeiri˜ na, G. Orkoulas, and M. E. Fisher, Soluble model fluids with complete scaling and Yang-Yang features, Phys. Rev. Lett.116, 040601 (2016); C. A. Cerdeiri˜ na and G. Ork- oulas, Compressible cell gas models for asymmetric fluid criticality, Phy...

  49. [49]

    R. J. Speedy, Comment on ’Supercooled and glassy wa- ter’, J. Phys.: Condens. Matter16, 6811 (2004)

  50. [50]

    Sastry, F

    The diverging nature of response functions at our su- percooled liquid spinodal contrasts with the behavior re- ported previously for other Ising-like models: S. Sastry, F. Sciortino, and H. E. Stanley, Limits of stability of the liquid phase in a lattice model with water-like prop- erties, J. Chem. Phys.98, 9863 (1993); S. S. Borick, P. G. Debenedetti, a...

  51. [51]

    F. H. Stillinger, Statistical mechanics of metastable mat- ter: Superheated and stretched liquid, Phys. Rev. E52, 4685 (1995)

  52. [52]

    In our assessment, an enhanced model is required to reasonably meet the low-Tbehavior of a full αp = 0 locus with the form of a closed loop like the one inferred from, e.g., P

    Curves with an isobaricv(T) maximum [ρ(T) minimum] indeed occur for a number of water force fields, but they fall beyond the capabilities of the five-state model ex- plored here. In our assessment, an enhanced model is required to reasonably meet the low-Tbehavior of a full αp = 0 locus with the form of a closed loop like the one inferred from, e.g., P. H...

  53. [53]

    J. R. Espinosa, J. L. F. Abascal L. F. Sedano, E. Sanz, and C. Vega, On the possible locus of the liquid–liquid critical point in real water from studies of supercooled water using the TIP4P/Ice model, J. Chem. Phys.158, 204505 (2023)

  54. [54]

    J. L. F. Abascal and C. Vega, Widom line and the liq- uid–liquid critical point for the TIP4P/2005 water model, J. Chem. Phys.133, 234502 (2010)

  55. [55]

    Sumi and H

    T. Sumi and H. Sekino, Effects of hydrophobic hydration on polymer chains immersed in supercooled water, RSC Adv.3, 12743 (2013)

  56. [56]

    M. A. Gonz´ alez, C. Valeriani, F. Caupin, and J. L. F. Abascal, J. Chem. Phys.145, 054505 (2016)

  57. [57]

    Data excerpted from NIST Chemistry WebBook: https://webbook.nist.gov/chemistry/

  58. [58]

    J. S. Rowlinson, The equation of state of dense systems, Rep. Prog. Phys.28, 169 (1965)

  59. [59]

    R. B. Griffiths and J. C. Wheeler, Critical points in mul- ticomponent systems, Phys. Rev. A2, 1047 (1970)

  60. [60]

    Mishima and H

    O. Mishima and H. E. Stanley, The relationship between liquid, supercooled, and glassy water, Nature (London) 396, 329 (1998)

  61. [61]

    P. G. Debenedetti, Supercooled and glassy water, J. Phys.: Condens. Matter15, R1669 (2003)

  62. [62]

    Handle, T

    H. Handle, T. Loerting, and F. Sciortino, Supercooled and glassy water: Metastable liquid(s), amorphous solid(s), and a no-man’s land, Proc. Nat. Acad Sci. U. S. A.114, 13336 (2017)

  63. [63]

    Parisi, P

    G. Parisi, P. Urbani, and F. ZamponiTheory of Simple Glasses(Cambridge University Press, Cambridge, 2020)