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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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The abstract, sentence by sentence
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
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| 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 |
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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
Papers citing it · 21 sentences without a confident label
Contests it 2 papers
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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
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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
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Finally, we compute the PBH masses using the critical scaling method [ref] for both formalisms.
Revisiting primordial black holes formation from preheating instabilities: the case of Starobinsky inflation · Numerical characterization of PBH formation · 0.99
Uses its data or values 1 paper
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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
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Numerical general relativistic simulations [ref] have demonstrated that the scaling of black hole mass with the proximity to the formation threshold, known to occur in near-critical gravitational collapse, also applies to PBH formation.
Primordial black holes through preheating instabilities in $\alpha$-attractor models · PBH mass · 0.96
Cites it as background 3 papers
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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
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Imploding scalar solutions have found application in models of gravitational collapse [ref] .
Hybrid imploding scalar and ads spacetime · Introduction · 0.95
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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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