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Self-Similar Scalar Field Collapse: Naked Singularities and Critical Behaviour
General Relativity and Quantum Cosmology · Submitted 16 Sep 1994
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The second class of solutions includes both black holes and naked singularities with a critical evolution (which is neither) interpolating between these two extremes.
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The abstract, sentence by sentence
Homothetic scalar field collapse is considered in this article. By making a suitable choice of variables the equations are reduced to an autonomous system. Then using a combination of numerical and analytic techniques it is shown that there are two classes of solutions. The first consists of solutions with a non-singular origin in which the scalar field collapses and disperses again. There is a singularity at one point of these solutions, however it is not visible to observers at finite radius. The second class of solutions includes both black holes and naked singularities with a critical evolution (which is neither) interpolating between these two extremes. The properties of these solutions are discussed in detail. The paper also contains some speculation about the significance of self-similarity in recent numerical studies.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Homothetic scalar field collapse is considered in this article. | background 0.55 | 0.55 | 0.02 | asserted 0.88 |
| s1 | By making a suitable choice of variables the equations are reduced to an autonomous system. | method 1.00 | 0.89 | 0.02 | asserted 1.00 |
| s2 | Then using a combination of numerical and analytic techniques it is shown that there are two classes of solutions. | result 0.56 | 0.94 | 0.21 | asserted 1.00 |
| s3 | The first consists of solutions with a non-singular origin in which the scalar field collapses and disperses again. | result 1.00 | 0.84 | 0.10 | asserted 1.00 |
| s4 | There is a singularity at one point of these solutions, however it is not visible to observers at finite radius. | result 0.91 | 0.79 | 0.07 | asserted 1.00 |
| s5 | The second class of solutions includes both black holes and naked singularities with a critical evolution (which is neither) interpolating between these two extremes. | result 1.00 | 0.85 | 0.56 | asserted 1.00 |
| s6 | The properties of these solutions are discussed in detail. | contribution 0.91 | 0.71 | 0.04 | asserted 0.77 |
| s7 | The paper also contains some speculation about the significance of self-similarity in recent numerical studies. | interpretation 0.78 | 0.42 | 0.03 | speculative 0.93 |
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The paper
Original abstract
Homothetic scalar field collapse is considered in this article. By making a suitable choice of variables the equations are reduced to an autonomous system. Then using a combination of numerical and analytic techniques it is shown that there are two classes of solutions. The first consists of solutions with a non-singular origin in which the scalar field collapses and disperses again. There is a singularity at one point of these solutions, however it is not visible to observers at finite radius. The second class of solutions includes both black holes and naked singularities with a critical evolution (which is neither) interpolating between these two extremes. The properties of these solutions are discussed in detail. The paper also contains some speculation about the significance of self-similarity in recent numerical studies.
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References
How the literature uses it
5 arXiv papers cite this in 14 sentences
Papers citing it · 11 sentences without a confident label
Cites it as background 3 papers
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The Roberts solution provides a useful analytic substitute: it is a closed-form CSS solution of the same Einstein-scalar system, supported by a massless scalar field, and captures several structural features of near-critical scalar collapse [ref] .
Quantum fate of the Choptuik naked singularity · The Roberts interior and its quantum horizon · 0.81
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This analytic CSS spacetime is closely related to the DSS solution first identified by Choptuik [ref] .
Quantum Critical Collapse Abhors a Naked Singularity · Introduction · 0.90
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Second, while we have focused on CSS-type spacetimes in $2+1$ and $3+1$ dimensions (i.e., the Garfinkle and Roberts solutions), many other exact solutions conjectured to model critical collapse exist in spherical symmetry [ref] .
Unveiling horizons in quantum critical collapse · Outlook · 0.88
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