2019
DOI: 10.1103/physrevd.100.024040
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Cut-and-paste for impulsive gravitational waves with Λ : The geometric picture

Abstract: Impulsive gravitational waves in Minkowski space were introduced by Roger Penrose at the end of the 1960s, and have been widely studied over the decades. Here we focus on non-expanding waves which later have been generalised to impulses travelling in all constantcurvature backgrounds, that is also the (anti-)de Sitter universe. While Penrose's original construction was based on his vivid geometric 'scissors-and-paste' approach in a flat background, until now a comparably powerful visualisation and understandin… Show more

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Cited by 14 publications
(29 citation statements)
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References 33 publications
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“…To date, an exact solution for a single propagating plane gravitational wave with λ > 0 has not been found. One cannot use Penrose's cut-and-paste method to find such a solution because this leads to wavefronts that are spherical or hyperboloidal when λ > 0 or λ < 0, respectively [14]. Thus, to try shed some light toward an analytic solution, we numerically evolve our system with λ > 0 and with one ingoing wave, whose wave profile approximates the Dirac delta function.…”
Section: An Impulsive Wavementioning
confidence: 99%
See 1 more Smart Citation
“…To date, an exact solution for a single propagating plane gravitational wave with λ > 0 has not been found. One cannot use Penrose's cut-and-paste method to find such a solution because this leads to wavefronts that are spherical or hyperboloidal when λ > 0 or λ < 0, respectively [14]. Thus, to try shed some light toward an analytic solution, we numerically evolve our system with λ > 0 and with one ingoing wave, whose wave profile approximates the Dirac delta function.…”
Section: An Impulsive Wavementioning
confidence: 99%
“…Penrose's cut-and-paste method [6,8], which cuts Minkowski space-time along a null hyperplane, shunts one half along the same surface and then pastes the two halves back together gives rise to a space-time with one impulsive gravitational wave (i.e., with a Dirac delta function wave profile). This has been generalized to non-zero, constant curvature backgrounds [9][10][11][12][13][14] where the wave fronts are topologically spherical for λ > 0 and hyperboloidal for λ < 0. There do not exist, however, closed form solutions to the full non-linear Einstein equations with λ = 0 that contain gravitational waves with plane symmetric wave fronts.…”
Section: Introductionmentioning
confidence: 99%
“…To date, an exact solution for a single propagating plane gravitational wave with λ > 0 has not been found. One cannot use Penrose's cut-and-paste method to find such a solution because this leads to wavefronts that are spherical or hyperboloidal when λ > 0 or λ < 0 respectively [16]. Thus, to try shed some light toward an analytic solution, we numerically evolve our system with λ > 0 and with one ingoing wave, whose wave profile approximates the Dirac delta function.…”
Section: An Impulsive Wavementioning
confidence: 99%
“…with a Dirac delta function wave profile.) This has been generalized to non-zero, constant curvature backgrounds [11,12,13,14,15,16] where the wave fronts are topologically spherical for λ > 0 and hyperboloidal for λ < 0. There do not exist however, closed form solutions to the full non-linear Einstein equations with λ = 0 that contain gravitational waves with plane symmetric wave fronts.…”
Section: Introductionmentioning
confidence: 99%
“…By means of this useful geometrical approach, Penrose was able to study certain classes of impulsive plane-fronted and sphericallyfronted waves in Minkowski's backgrounds. Later works of works of Podolskỳ et al [27], [30], [28] apply this method to generate spacetimes whose metric again contains a Dirac delta function with support on the null hypersurface. The most general construction so far describes pp-waves with additional gyratonic terms [30].…”
Section: Introductionmentioning
confidence: 99%