Memory effects in Kundt wave spacetimes

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 whi...

Full description

Bibliographic Details
Main Authors: Indranil Chakraborty, Sayan Kar
Format: Article
Language:English
Published: Elsevier 2020-09-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269320304147
id doaj-1c6e1908f5664ea3b39f5647c18933a0
record_format Article
spelling doaj-1c6e1908f5664ea3b39f5647c18933a02020-11-25T02:58:56ZengElsevierPhysics Letters B0370-26932020-09-01808135611Memory effects in Kundt wave spacetimesIndranil Chakraborty0Sayan Kar1Centre for Theoretical Studies, Indian Institute of Technology Kharagpur, 721 302, India; Corresponding author.Centre for Theoretical Studies, Indian Institute of Technology Kharagpur, 721 302, India; Department of Physics, Indian Institute of Technology Kharagpur, 721 302, IndiaMemory 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.http://www.sciencedirect.com/science/article/pii/S0370269320304147
collection DOAJ
language English
format Article
sources DOAJ
author Indranil Chakraborty
Sayan Kar
spellingShingle Indranil Chakraborty
Sayan Kar
Memory effects in Kundt wave spacetimes
Physics Letters B
author_facet Indranil Chakraborty
Sayan Kar
author_sort Indranil Chakraborty
title Memory effects in Kundt wave spacetimes
title_short Memory effects in Kundt wave spacetimes
title_full Memory effects in Kundt wave spacetimes
title_fullStr Memory effects in Kundt wave spacetimes
title_full_unstemmed Memory effects in Kundt wave spacetimes
title_sort memory effects in kundt wave spacetimes
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2020-09-01
description 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.
url http://www.sciencedirect.com/science/article/pii/S0370269320304147
work_keys_str_mv AT indranilchakraborty memoryeffectsinkundtwavespacetimes
AT sayankar memoryeffectsinkundtwavespacetimes
_version_ 1724704386239692800