2018
DOI: 10.1088/1361-6382/aaeca5
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Safely smoothing spacetime: backreaction in relativistic cosmological simulations

Abstract: A persistent theme in the study of dark energy is the question of whether it really exists or not. It is often claimed that we are mis-calculating the cosmological model by neglecting the effects associated with averaging over large-scale structures. In the Newtonian approximation this is clear: there is no effect. Within the full relativistic picture this remains an important open question, owing to the complex mathematics involved. We study this issue using numerical N-body simulations which account for all … Show more

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Cited by 42 publications
(52 citation statements)
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“…Our numerical experiment provides conclusive evidence that the relativistic evolution of inhomogeneities, once consistently combined with the kinematics of light propagation on the inhomogeneous spacetime geometry, does not lead to an unexpectedly large bias of the distance-redshift correlation. This corroborates the conclusions of [1][2][3][4][5][6]28]. On the other hand, inhomogeneities introduce a significant non-Gaussian scatter that can give a large standard error on the mean when only a small sample of sources is available.…”
Section: Discussionsupporting
confidence: 87%
“…Our numerical experiment provides conclusive evidence that the relativistic evolution of inhomogeneities, once consistently combined with the kinematics of light propagation on the inhomogeneous spacetime geometry, does not lead to an unexpectedly large bias of the distance-redshift correlation. This corroborates the conclusions of [1][2][3][4][5][6]28]. On the other hand, inhomogeneities introduce a significant non-Gaussian scatter that can give a large standard error on the mean when only a small sample of sources is available.…”
Section: Discussionsupporting
confidence: 87%
“…For some of the largest structures in our Universe that have been observationally well-characterized, we find that nonlinear effects can approach the percent level even in harmonic and Newtonian gauges, while linear theory is entirely unable describe the synchronous gauge metric. These findings coincide with expectations: it is well-known that the amplitude of metric perturbations can vary significantly between gauges or "slicing conditions" [15], as noted in other approximate and analytic treatments [16,17] as well. For density perturbations of cosmologically common amplitudes in synchronous gauge, the metric amplitude scales roughly with the density contrast δ ρ , and can therefore become quite large, while in harmonic slicing and a quasi-Newtonian gauge, metric perturbations remain small.…”
Section: Introductionsupporting
confidence: 89%
“…However, as pointed out many times before (e.g. [44,53,62,65,66,[80][81][82]), a possible issue with such a procedure is that observations are mainly made on the light cone. Therefore, spatially averaged quantities (including backreaction terms) are only relevant if they can be related to observables in a sensible manner.…”
Section: Average Light Propagationmentioning
confidence: 99%