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Critical phenomena in perfect fluids

General Relativity and Quantum Cosmology · Submitted 16 Dec 1998

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim In addition, we find strong evidence that globally regular critical solutions do exist for 1.89 < Gamma <= 2$, that the sonic point for Gamma_dn = 1.8896244 is a degenerate node, and that the sonic points for Gamma >Gamma_dn are nodal points rather than focal points as previously reported.

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arXiv IDgr-qc/9812053 (version 2)
Pith IDCBUK5KCU, Pith's permanent record of this paper and its review
CitationDavid W. Neilsen, Matthew W. Choptuik. "Critical phenomena in perfect fluids." arXiv:gr-qc/9812053 (1998). https://pith.science/paper/CBUK5KCU
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 6,581 input tokens, $0.0003 reported.

What the abstract itself states, as probabilities: claims first 0.06 · states limitation 0.36 · human participants 0.01 · controlled comparison 0.05 · randomized assignment 0.01 · states quantitative result 0.97 · compares with prior results 0.97 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

We investigate the gravitational collapse of a spherically symmetric, perfect fluid with equation of state P = (Gamma -1)rho. We restrict attention to the ultrarelativistic (``kinetic-energy-dominated'', ``scale-free'') limit where black hole formation is anticipated to turn on at infinitesimal black hole mass (Type II behavior). Critical solutions (those which sit at the threshold of black hole formation in parametrized families of collapse) are found by solving the system of ODEs which result from a self-similar ansatz, and by solving the full Einstein/fluid PDEs in spherical symmetry. These latter PDE solutions (``simulations'') extend the pioneering work of Evans and Coleman (Gamma = 4/3) and verify that the continuously self-similar solutions previously found by Maison and Hara et al for $1.05 < Gamma < 1.89 are (locally) unique critical solutions. In addition, we find strong evidence that globally regular critical solutions do exist for 1.89 < Gamma <= 2$, that the sonic point for Gamma_dn = 1.8896244 is a degenerate node, and that the sonic points for Gamma >Gamma_dn are nodal points rather than focal points as previously reported. We also find a critical solution for Gamma = 2, and present evidence that it is continuously self-similar and Type II. Mass-scaling exponents for all of the critical solutions are calculated by evolving near-critical initial data, with results which confirm and extend previous calculations based on linear perturbation theory. Finally, we comment on critical solutions generated with an ideal-gas equation of state.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We investigate the gravitational collapse of a spherically symmetric, perfect fluid with equation of state P = (Gamma -1)rho. contribution 0.83 0.88 0.03 asserted 0.87
s1 We restrict attention to the ultrarelativistic (``kinetic-energy-dominated'', ``scale-free'') limit where black hole formation is anticipated to turn on at infinitesimal black hole mass (Type II behavior). limitation 0.43 0.40 0.05 hedged possibility 0.86
s2 Critical solutions (those which sit at the threshold of black hole formation in parametrized families of collapse) are found by solving the system of ODEs which result from a self-similar ansatz, and by solving the full Einstein/fluid PDEs in spherical symmetry. method 0.97 0.93 0.07 asserted 1.00
s3 These latter PDE solutions (``simulations'') extend the pioneering work of Evans and Coleman (Gamma = 4/3) and verify that the continuously self-similar solutions previously found by Maison and Hara et al for $1.05 < Gamma < 1.89 are (locally) unique critical solutions. result 0.72 0.81 0.15 asserted 1.00
s4 In addition, we find strong evidence that globally regular critical solutions do exist for 1.89 < Gamma <= 2$, that the sonic point for Gamma_dn = 1.8896244 is a degenerate node, and that the sonic points for Gamma >Gamma_dn are nodal points rather than focal points as previously reported. result 1.00 0.96 0.26 asserted 0.71
s5 We also find a critical solution for Gamma = 2, and present evidence that it is continuously self-similar and Type II. result 0.94 0.97 0.17 asserted 0.94
s6 Mass-scaling exponents for all of the critical solutions are calculated by evolving near-critical initial data, with results which confirm and extend previous calculations based on linear perturbation theory. result 0.86 0.96 0.10 asserted 1.00
s7 Finally, we comment on critical solutions generated with an ideal-gas equation of state. contribution 0.38 0.43 0.04 unclear 0.89

What kind of paper the classifier reports this is: simulation study 0.98 · evidence from simulation or computation 1.00.

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  • arXiv listing abstract v2
not examined
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  • figures and tables
  • references and citing sentences
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  • S sections
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  • C citations
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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

We investigate the gravitational collapse of a spherically symmetric, perfect fluid with equation of state P = (Gamma -1)rho. We restrict attention to the ultrarelativistic (``kinetic-energy-dominated'', ``scale-free'') limit where black hole formation is anticipated to turn on at infinitesimal black hole mass (Type II behavior). Critical solutions (those which sit at the threshold of black hole formation in parametrized families of collapse) are found by solving the system of ODEs which result from a self-similar ansatz, and by solving the full Einstein/fluid PDEs in spherical symmetry. These latter PDE solutions (``simulations'') extend the pioneering work of Evans and Coleman (Gamma = 4/3) and verify that the continuously self-similar solutions previously found by Maison and Hara et al for $1.05 < Gamma < 1.89 are (locally) unique critical solutions. In addition, we find strong evidence that globally regular critical solutions do exist for 1.89 < Gamma <= 2$, that the sonic point for Gamma_dn = 1.8896244 is a degenerate node, and that the sonic points for Gamma >Gamma_dn are nodal points rather than focal points as previously reported. We also find a critical solution for Gamma = 2, and present evidence that it is continuously self-similar and Type II. Mass-scaling exponents for all of the critical solutions are calculated by evolving near-critical initial data, with results which confirm and extend previous calculations based on linear perturbation theory. Finally, we comment on critical solutions generated with an ideal-gas equation of state.

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References
How the literature uses it

19 arXiv papers cite this in 29 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 21 sentences without a confident label

Contests it 2 papers
  • As Ori and Piran before [ref] , he claimed that there are no regular CSS solutions for $k>0.89$, but Neilsen and Choptuik [ref] have found CSS critical solutions for all values of $k$ right up to 1, both in collapse simulations and by making a CSS ansatz.

    Critical phenomena in gravitational collapse · Spherical symmetry · contest 0.80

  • As [ref] before, he claimed that there are no regular CSS solutions for $k>0.89$, but [ref] have found CSS critical solutions for all values of $k$ right up to 1, both in collapse simulations and by making a CSS ansatz.

    Critical Phenomena in Gravitational Collapse · The asymptotically flat case · contest 0.84

Uses its method or tool 1 paper
Uses its data or values 1 paper
  • The PBH mass $M_PBH(ν)$ is proportional to the horizon mass at horizon-crossing time, $M_H(t_m)$, according to the relation [ref] [equation] In this equation the horizon mass at horizon-crossing time is given by the equation $M_H(t_m) = 1/2H_m$ while the factor $(ν-ν_c)^γ$ is the scaling law for critical collapse (extracted from numerical simulation, and with $γ̃≃0.36$ in the case of radiation [ref] ) while $𝒦 = O(1)$.

    Solving peak theory in the presence of local non-gaussianities · Threshold for gravitational collapse into black holes · 0.85

Cites it as support 1 paper
Cites it as background 3 papers
  • Since Choptuik's discovery, this framework has been generalized to a wide variety of matter models in spherical symmetry [ref] , revealing extremely rich phase structures depending on the number of dimensions and the type of matter content.

    Unveiling horizons in quantum critical collapse · Introduction · 0.85

  • Imploding scalar solutions have found application in models of gravitational collapse [ref] .

    Hybrid imploding scalar and ads spacetime · Introduction · 0.95

  • For example, the previous work has been extended to massive scalar fields [ref] , the gravitational collapse of radiation [ref] and perfect fluid [ref] , a complex scalar field with angular momentum [ref] , K-essence models [ref] , the Einstein-Massless-Dirac system [ref] , and massive vector field [ref] , to mention some of the many investigations carried out to date.

    Critical collapse for the Starobinsky $R^2$ model · Introduction · 0.80

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