2021
DOI: 10.1007/s41614-021-00055-z
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Cosmological Vlasov–Poisson equations for dark matter

Abstract: The cosmic large-scale structures of the Universe are mainly the result of the gravitational instability of initially small-density fluctuations in the dark-matter distribution. Dark matter appears to be initially cold and behaves as a continuous and collisionless medium on cosmological scales, with evolution governed by the gravitational Vlasov–Poisson equations. Cold dark matter can accumulate very efficiently at focused locations, leading to a highly non-linear filamentary network with extreme matter densit… Show more

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Cited by 16 publications
(9 citation statements)
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References 208 publications
(246 reference statements)
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“…Moreover, since LPT is a Taylor series in powers of a, the temporal regime of convergence is spanned by |a| < a , where the radius of convergence a is set by the nearest singularity(ies) in the complex-time plane around the expansion point a = 0. In the case of spherical symmetry, the nearest singularity occurs at the real-valued collapse time a where, specifically, the velocity v = ẋ blows up [25,61]. This explains the exact coincidence between the collapse time and the loss of convergence in the case of spherical symmetry.…”
Section: Lagrangian Perturbation Theorymentioning
confidence: 94%
See 1 more Smart Citation
“…Moreover, since LPT is a Taylor series in powers of a, the temporal regime of convergence is spanned by |a| < a , where the radius of convergence a is set by the nearest singularity(ies) in the complex-time plane around the expansion point a = 0. In the case of spherical symmetry, the nearest singularity occurs at the real-valued collapse time a where, specifically, the velocity v = ẋ blows up [25,61]. This explains the exact coincidence between the collapse time and the loss of convergence in the case of spherical symmetry.…”
Section: Lagrangian Perturbation Theorymentioning
confidence: 94%
“…Cosmological perturbation theory (CPT; [21][22][23][24][25]) provides highly accurate predictions on large cosmological scales, and in particular plays a crucial role in connecting early-with latetime cosmology, such as by providing initial conditions for numerical simulations [26][27][28][29][30]. However, CPT struggles to accurately predict the small-scale collapse to gravitationally bound structures, a process that is intimately tied to the shellcrossing singularity-the crossing of trajectories of collisionless matter, which comes with extreme matter densities.…”
Section: Introductionmentioning
confidence: 99%
“…In order to understand the results exposed above, we will use the LPT formalism [6,13,16] to compute approximate expressions for the power spectra that go into equation (3.3) and their variances; this will allow us to see what are the effects of fixing or pairing on the structure of these quantities. Let us call F (q) a field in Lagrangian space such that…”
Section: Theoretical Explorationmentioning
confidence: 99%
“…Nonetheless, there exist by now various algorithms that can incorporate the gravitational interactions efficiently; to a good approximation even after the appearance of the first singularities [32,33]; see e.g. [34] for a review.…”
Section: Discussionmentioning
confidence: 99%