2014
DOI: 10.1103/physrevd.89.123502
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Black hole universe with a cosmological constant

Abstract: Time evolution of a black hole lattice universe with a positive cosmological constant Λ is simulated. The vacuum Einstein equations are numerically solved in a cubic box with a black hole in the center. Periodic boundary conditions on all pairs of opposite faces are imposed. Configurations of marginally trapped surfaces are analyzed. We describe the time evolution of not only black hole horizons, but also cosmological horizons. Defining the effective scale factor by using the area of a surface of the cubic box… Show more

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Cited by 41 publications
(51 citation statements)
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“…δ O r A corresponds to the position drift measured with respect to inertially dragged fixed directions. Combining (74) and (73) yields…”
Section: Position Drift Formulamentioning
confidence: 99%
“…δ O r A corresponds to the position drift measured with respect to inertially dragged fixed directions. Combining (74) and (73) yields…”
Section: Position Drift Formulamentioning
confidence: 99%
“…In order to avoid a highly distorted time slices for the calculation of the surface area, similarly to Refs. [11,16], we calculate the surface area S on the constant proper time slice for the set of observers fixed at grid points. Thus, the area S is given as a function of the proper time τ .…”
Section: Time Evolutionmentioning
confidence: 99%
“…Numerical simulations of spacetime dynamics in cosmological settings have been actively performed in recent years. One main motivation to simulate the cosmological nonlinear dynamics is to quantify the effect of the non-linear small scale inhomogeneity on the global expansion law of the universe [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16]. Another significant motivation comes from primordial black holes [17,18].…”
Section: Introductionmentioning
confidence: 99%