2019
DOI: 10.1088/1475-7516/2019/06/018
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Suitable initial conditions for Newtonian simulations with massive neutrinos

Abstract: Initial conditions for cosmological N-body simulations are usually calculated by rescaling the present day linear power spectrum obtained from an Einstein-Boltzmann solver to the initial time employing the scale-independent matter growth function. For the baseline ΛCDM model, this has been shown to be consistent with General Relativity (GR) even in the presence of relativistic species such as photons. We show that this approach is not feasible in cosmologies with massive neutrinos and present an alternative me… Show more

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Cited by 10 publications
(19 citation statements)
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“…The second feature is the non-vanishing slope at the final time, which produces a little bump around z = 1. Our result differs from the previously presented backwards method in [45], which has a different slope at the final time and relies on initialising the simulation with specific initial conditions. Our new solution combines the ease to use common backscaling initial conditions with generally small values for H T , implying that the particle positions updates are small.…”
Section: Backwards Newtonian Motion Gaugescontrasting
confidence: 71%
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“…The second feature is the non-vanishing slope at the final time, which produces a little bump around z = 1. Our result differs from the previously presented backwards method in [45], which has a different slope at the final time and relies on initialising the simulation with specific initial conditions. Our new solution combines the ease to use common backscaling initial conditions with generally small values for H T , implying that the particle positions updates are small.…”
Section: Backwards Newtonian Motion Gaugescontrasting
confidence: 71%
“…In backscaling however, we utilise the present time power spectrum to initialise the simulation which makes it natural to fix the residual gauge freedom at the final time and solve the ODE backwards. This defines the term of a backwards Newtonian motion gauge and in [45] we have concluded that we can set H T (τ f ) = 3ζ(τ f ) and the derivative ḢT (τ f ) = 3 ζ(τ f ) such that the gauge formally agrees with the N-boisson gauge at the final time:…”
Section: Backwards Newtonian Motion Gaugesmentioning
confidence: 94%
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“…In this paper, we run Newtonian simulations exploiting the Newtonian motion gauge approach, thereby allowing us to include massive neutrinos in terms of a post-processing, while delivering a solution that is in accordance with the weak-field limit of general relativity. The specific technical setup necessary for this has been developed especially by the references [38] and [39]. We summarise the general idea of the approach in the following section, while more specific details needed for the implementation are outlined in section 3.…”
Section: Introductionmentioning
confidence: 99%