Abstract

Memory effects in the exact Kundt wave spacetimes are shown to arise in the behaviour of geodesics in such spacetimes. The types of Kundt spacetimes we consider here are direct products of the form H2×M(1,1) and S2×M(1,1). Both geometries have constant scalar curvature. We consider a scenario in which initial velocities of the transverse geodesic coordinates are set to zero (before the arrival of the pulse) in a spacetime with non-vanishing background curvature. We look for changes in the separation between pairs of geodesics caused by the pulse. Any relative change observed in the position and velocity profiles of geodesics, after the burst, can be solely attributed to the wave (hence, a memory effect). For constant negative curvature, we find there is permanent change in the separation of geodesics after the pulse has departed. Thus, there is displacement memory, though no velocity memory is found. In the case of constant positive scalar curvature (Plebański–Hacyan spacetimes), we find both displacement and velocity memory along one direction. In the other direction, a new kind of memory (which we term as frequency memory effect) is observed where the separation between the geodesics shows periodic oscillations once the pulse has left. We also carry out similar analyses for spacetimes with a non-constant scalar curvature, which may be positive or negative. The results here seem to qualitatively agree with those for constant scalar curvature, thereby suggesting a link between the nature of memory and curvature.

Highlights

  • The study of memory effects have resurfaced recently since a suggested possibility of detection in advanced detectors like aLIGO, LISA and PTA [1],[2]

  • Garfinkle and several others considered massless fields propagating to null infinity [9] and, introduced an electromagnetic memory effect [10] as well as a neutrino memory effect [11]

  • Displacement and velocity memory effects have been addressed by solving geodesic equations for sandwich wave spacetimes [20,21,22]

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Summary

Introduction

The study of memory effects have resurfaced recently since a suggested possibility of detection in advanced detectors like aLIGO, LISA and PTA [1],[2]. Displacement and velocity memory effects have been addressed by solving geodesic equations for sandwich wave spacetimes [20,21,22]. We study memory effects in spacetimes where the two regions separated by the pulse have finite curvature.

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