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Developments of initial data on big bang singularities for the Einstein-nonlinear scalar field equations
General Relativity and Quantum Cosmology · Submitted 25 Sep 2024
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We prove that given initial data on the singularity for the Einstein-nonlinear scalar field equations in 4 spacetime dimensions, as defined by Ringstr\"om, there is a corresponding unique development of the data.
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The abstract, sentence by sentence
In a recent work, Ringstr\"om proposed a geometric notion of initial data on big bang singularities. Moreover, he conjectured that initial data on the singularity could be used to parameterize quiescent solutions to Einstein's equations; that is, roughly speaking, solutions whose leading order asymptotics are convergent. We prove that given initial data on the singularity for the Einstein-nonlinear scalar field equations in 4 spacetime dimensions, as defined by Ringstr\"om, there is a corresponding unique development of the data. We do not assume any symmetry or analyticity, and we allow for arbitrary closed spatial topology. Our results thus present an important step towards resolving Ringstr\"om's conjecture. Furthermore, our results show that the Einstein-nonlinear scalar field equations have a geometric singular initial value problem formulation, which is analogous to the classical result by Choquet-Bruhat and Geroch for initial data on a Cauchy hypersurface. In the literature, there are two conditions which are expected to ensure that quiescent behavior occurs. The first one is an integrability condition on a special spatial frame. The second one is an algebraic condition on the eigenvalues of the expansion normalized Weingarten map associated with a foliation of the spacetime near the singularity. Our result is the first such result where both possibilities are allowed. That is, we allow for the first condition to ensure quiescence in one region of space and for the second condition to take over in the region where the first one is violated. This fact allows for our results to include the vacuum setting.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In a recent work, Ringstr\"om proposed a geometric notion of initial data on big bang singularities. | background 1.00 | 0.03 | 0.02 | asserted 1.00 |
| s1 | Moreover, he conjectured that initial data on the singularity could be used to parameterize quiescent solutions to Einstein's equations; that is, roughly speaking, solutions whose leading order asymptotics are convergent. | background 0.99 | 0.03 | 0.03 | speculative 0.58 |
| s2 | We prove that given initial data on the singularity for the Einstein-nonlinear scalar field equations in 4 spacetime dimensions, as defined by Ringstr\"om, there is a corresponding unique development of the data. | result 0.93 | 0.96 | 0.92 | asserted 1.00 |
| s3 | We do not assume any symmetry or analyticity, and we allow for arbitrary closed spatial topology. | contribution 0.65 | 0.82 | 0.04 | asserted 1.00 |
| s4 | Our results thus present an important step towards resolving Ringstr\"om's conjecture. | interpretation 1.00 | 0.54 | 0.14 | asserted 0.86 |
| s5 | Furthermore, our results show that the Einstein-nonlinear scalar field equations have a geometric singular initial value problem formulation, which is analogous to the classical result by Choquet-Bruhat and Geroch for initial data on a Cauchy hypersurface. | interpretation 0.90 | 0.94 | 0.19 | asserted 1.00 |
| s6 | In the literature, there are two conditions which are expected to ensure that quiescent behavior occurs. | background 1.00 | 0.04 | 0.02 | hedged possibility 0.74 |
| s7 | The first one is an integrability condition on a special spatial frame. | background 1.00 | 0.05 | 0.02 | asserted 0.89 |
| s8 | The second one is an algebraic condition on the eigenvalues of the expansion normalized Weingarten map associated with a foliation of the spacetime near the singularity. | background 1.00 | 0.06 | 0.02 | asserted 0.71 |
| s9 | Our result is the first such result where both possibilities are allowed. | contribution 0.69 | 0.90 | 0.08 | asserted 1.00 |
| s10 | That is, we allow for the first condition to ensure quiescence in one region of space and for the second condition to take over in the region where the first one is violated. | contribution 0.51 | 0.91 | 0.06 | asserted 0.95 |
| s11 | This fact allows for our results to include the vacuum setting. | interpretation 0.92 | 0.81 | 0.05 | asserted 0.97 |
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The paper
Original abstract
In a recent work, Ringstr\"om proposed a geometric notion of initial data on big bang singularities. Moreover, he conjectured that initial data on the singularity could be used to parameterize quiescent solutions to Einstein's equations; that is, roughly speaking, solutions whose leading order asymptotics are convergent. We prove that given initial data on the singularity for the Einstein-nonlinear scalar field equations in 4 spacetime dimensions, as defined by Ringstr\"om, there is a corresponding unique development of the data. We do not assume any symmetry or analyticity, and we allow for arbitrary closed spatial topology. Our results thus present an important step towards resolving Ringstr\"om's conjecture. Furthermore, our results show that the Einstein-nonlinear scalar field equations have a geometric singular initial value problem formulation, which is analogous to the classical result by Choquet-Bruhat and Geroch for initial data on a Cauchy hypersurface. In the literature, there are two conditions which are expected to ensure that quiescent behavior occurs. The first one is an integrability condition on a special spatial frame. The second one is an algebraic condition on the eigenvalues of the expansion normalized Weingarten map associated with a foliation of the spacetime near the singularity. Our result is the first such result where both possibilities are allowed. That is, we allow for the first condition to ensure quiescence in one region of space and for the second condition to take over in the region where the first one is violated. This fact allows for our results to include the vacuum setting.
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References
How the literature uses it
2 arXiv papers cite this in 10 sentences
Papers citing it · 7 sentences without a confident label
Compares with it 2 papers
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However, the assumptions in [ref] are such that the following theorem is not a special case of the results of [ref] .
On the structure of big bang singularities in spatially homogenous solutions to the Einstein non-linear scalar field equations · Developments inducing data on the singularity · 0.97
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The energy argument in [ref] is closely related to the one employed in [ref] .
A localized construction of Kasner-like singularities · Asymptotic data in 1+3 vacuum · 0.86
Cites it as background 1 paper
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Numerous constructions have been achieved in various settings [ref] .
A localized construction of Kasner-like singularities · Introduction · 0.84
What it cites · 17 sentences without a confident label
Uses the method or tool of 3 papers
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This is accomplished by using Einstein's equations, with arguments resembling those of [ref] .
Initial data on big bang singularities · Strategy for the proof · 0.98
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The argument is similar to those used in [ref] .
2309.11370 · Proofs of Theorems [ref] and [ref] · 0.96
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However, by an argument similar to [ref] , there is a finite covering space of $Σ$ such that, if we pull back the initial data, the pullback of $$ by the covering map has a global frame of eigenvectors.
Wave equations on silent big bang backgrounds · Developments of initial data on the singularity · 0.82
Compares with 2 papers
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If we compare Definition [ref] with [ref] , we note that the definitions of the expansion normalized induced metric differ.
Initial data on big bang singularities · Main results · 1.00
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By contrast, our definition of $$ corresponds to that of [ref] , which has the advantage of being frame independent, and of being independent of the initial data on the singularity.
2309.11370 · Main results · 0.97
Cites as support 2 papers
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The necessity of this condition is shown in [ref] .
Initial data on big bang singularities · Main results · 0.97
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That this condition should be sufficient is suggested by [ref] , necessity is discussed in [ref] .
2101.04955 · Related works · 0.97
Cites as background 8 papers
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In [ref] , Ringström proposed a geometric notion of initial data on big bang singularities.
Initial data on big bang singularities · Introduction · 0.94
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What is remarkable about [ref] is that it does not make reference to any background solution.
2309.11370 · Related works · 0.85
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For other recent results on stability of big bang singularities see [ref] .
Past stability of FLRW solutions to the Einstein-Euler-scalar field equations and their big bang singularites · Related works · 0.99
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