Abstract. The numerical investigation of wave propagation in the asymptotic domain of Kerr spacetime has only recently been possible thanks to the construction of suitable hyperboloidal coordinates. The asymptotics revealed a puzzle in the decay rates of scalar fields: the late-time rates seemed to depend on whether finite distance observers are in the strong field domain or far away from the rotating black hole. In this paper we study late-time decay rates using a horizon-penetrating, hyperboloidal slicing with transmitting layers attached to a compact domain in Boyer–Lindquist coordinates. The technical construction of transmitting layers for Kerr spacetime should be useful in future studies of wave propagation. We discuss splitting of lo...
We derive the Teukolsky equation for perturbations of a Kerr spacetime when the spacetime metric is ...
This paper investigates the decay properties of solutions to the massive linear wave equationgψ+ αl2...
Outside a black hole, perturbation fields die off in time as 1/t n. For spherical holes n = 2ℓ + 3 w...
16 pagesInternational audienceThe numerical investigation of wave propagation in the asymptotic doma...
We present new results from two codes, using finite differencing and pseudo-spectral methods for the...
We present an analytic method for calculating the late-time tails of a linear scalar field outside a...
We investigate the behavior of a dynamical scalar field on a fixed Kerr background in Kerr-Schild co...
We present a new analytic approach for the study of late time evolution of linear test-fields, propa...
We study analytically, via the Newman-Penrose formalism, the late-time decay of linear electromagnet...
We investigate the late-time behavior of a scalar field on a fixed Kerr background using a 2 + 1 dim...
We study analytically, via the Newman-Penrose formalism, the late time decay of scalar, electromagne...
In this work, we compute the precise late-time asymptotics for the scalar field in the interior of a...
Abstract. Energy and decay estimates for the wave equation on the exterior region of slowly rotating...
We present a new analytic approach for the study of late time evolution of linear test-fields, propa...
This note discusses the late-time decay of perturbations outside ex-tremal Reissner-Nordstrom black ...
We derive the Teukolsky equation for perturbations of a Kerr spacetime when the spacetime metric is ...
This paper investigates the decay properties of solutions to the massive linear wave equationgψ+ αl2...
Outside a black hole, perturbation fields die off in time as 1/t n. For spherical holes n = 2ℓ + 3 w...
16 pagesInternational audienceThe numerical investigation of wave propagation in the asymptotic doma...
We present new results from two codes, using finite differencing and pseudo-spectral methods for the...
We present an analytic method for calculating the late-time tails of a linear scalar field outside a...
We investigate the behavior of a dynamical scalar field on a fixed Kerr background in Kerr-Schild co...
We present a new analytic approach for the study of late time evolution of linear test-fields, propa...
We study analytically, via the Newman-Penrose formalism, the late-time decay of linear electromagnet...
We investigate the late-time behavior of a scalar field on a fixed Kerr background using a 2 + 1 dim...
We study analytically, via the Newman-Penrose formalism, the late time decay of scalar, electromagne...
In this work, we compute the precise late-time asymptotics for the scalar field in the interior of a...
Abstract. Energy and decay estimates for the wave equation on the exterior region of slowly rotating...
We present a new analytic approach for the study of late time evolution of linear test-fields, propa...
This note discusses the late-time decay of perturbations outside ex-tremal Reissner-Nordstrom black ...
We derive the Teukolsky equation for perturbations of a Kerr spacetime when the spacetime metric is ...
This paper investigates the decay properties of solutions to the massive linear wave equationgψ+ αl2...
Outside a black hole, perturbation fields die off in time as 1/t n. For spherical holes n = 2ℓ + 3 w...