Figure 22: Left: Elementary cells for the 8-BH configuration, projected to 
. The marginal
surface corresponding to the BH at infinity encompasses the whole configuration. Note that the 8
cubical lattice cells are isometric after the conformal rescaling. Right: Several measures of scaling in
the eight-BH universe, as functions of proper time 
, plotted against a possible identification of the
corresponding FLRW model (see Ref. [86] for details). All the quantities have been renormalized to
their respective values at 
. Images reproduced with permission from [86], copyright by IOP.
All rights reserved.
. The marginal
surface corresponding to the BH at infinity encompasses the whole configuration. Note that the 8
cubical lattice cells are isometric after the conformal rescaling. Right: Several measures of scaling in
the eight-BH universe, as functions of proper time , plotted against a possible identification of the
corresponding FLRW model (see Ref. [86] for details). All the quantities have been renormalized to
their respective values at . Images reproduced with permission from [86], copyright by IOP.
All rights reserved.Vitor Cardoso and Leonardo Gualtieri and Carlos Herdeiro and Ulrich Sperhake, "Exploring New Physics Frontiers Through Numerical
Relativity",
Living Rev. Relativity, 18 (2015), 1, doi:10.1007/lrr-2015-1, URL (accessed <date>): http://www.livingreviews.org/lrr-2015-1.![]()
This work is licensed under a Creative Commons Attribution 4.0 International License.
© The author(s), except where otherwise noted.
Living Rev. Relativity, 18 (2015), 1, doi:10.1007/lrr-2015-1, URL (accessed <date>): http://www.livingreviews.org/lrr-2015-1.