Kundt geometries and memory effects in the Brans–Dicke theory of gravity

Abstract Memory effects are studied in the simplest scalar–tensor theory, the Brans–Dicke (BD) theory. To this end, we introduce, in BD theory, novel Kundt spacetimes (without and with gyratonic terms), which serve as backgrounds for the ensuing analysis on memory. The BD parameter $$\omega $$ ω and...

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Main Authors: Siddhant Siddhant, Indranil Chakraborty, Sayan Kar
Format: Article
Language:English
Published: SpringerOpen 2021-04-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-021-09118-4
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spelling doaj-24b8cb9a2a95459dbd9718bfcfd802932021-04-25T11:44:01ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-04-0181411610.1140/epjc/s10052-021-09118-4Kundt geometries and memory effects in the Brans–Dicke theory of gravitySiddhant Siddhant0Indranil Chakraborty1Sayan Kar2Department of Physics, Indian Institute of Technology KharagpurDepartment of Physics, Indian Institute of Technology KharagpurDepartment of Physics, Indian Institute of Technology KharagpurAbstract Memory effects are studied in the simplest scalar–tensor theory, the Brans–Dicke (BD) theory. To this end, we introduce, in BD theory, novel Kundt spacetimes (without and with gyratonic terms), which serve as backgrounds for the ensuing analysis on memory. The BD parameter $$\omega $$ ω and the scalar field ( $$\phi $$ ϕ ) profile, expectedly, distinguishes between different solutions. Choosing specific localised forms for the free metric functions $$H'(u)$$ H ′ ( u ) (related to the wave profile) and J(u) (the gyraton) we obtain displacement memory effects using both geodesics and geodesic deviation. An interesting and easy-to-understand exactly solvable case arises when $$\omega =-2$$ ω = - 2 (with J(u) absent) which we discuss in detail. For other $$\omega $$ ω (in the presence of J or without), numerically obtained geodesics lead to results on displacement memory which appear to match qualitatively with those found from a deviation analysis. Thus, the issue of how memory effects in BD theory may arise and also differ from their GR counterparts, is now partially addressed, at least theoretically, within the context of this new class of Kundt geometries.https://doi.org/10.1140/epjc/s10052-021-09118-4
collection DOAJ
language English
format Article
sources DOAJ
author Siddhant Siddhant
Indranil Chakraborty
Sayan Kar
spellingShingle Siddhant Siddhant
Indranil Chakraborty
Sayan Kar
Kundt geometries and memory effects in the Brans–Dicke theory of gravity
European Physical Journal C: Particles and Fields
author_facet Siddhant Siddhant
Indranil Chakraborty
Sayan Kar
author_sort Siddhant Siddhant
title Kundt geometries and memory effects in the Brans–Dicke theory of gravity
title_short Kundt geometries and memory effects in the Brans–Dicke theory of gravity
title_full Kundt geometries and memory effects in the Brans–Dicke theory of gravity
title_fullStr Kundt geometries and memory effects in the Brans–Dicke theory of gravity
title_full_unstemmed Kundt geometries and memory effects in the Brans–Dicke theory of gravity
title_sort kundt geometries and memory effects in the brans–dicke theory of gravity
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2021-04-01
description Abstract Memory effects are studied in the simplest scalar–tensor theory, the Brans–Dicke (BD) theory. To this end, we introduce, in BD theory, novel Kundt spacetimes (without and with gyratonic terms), which serve as backgrounds for the ensuing analysis on memory. The BD parameter $$\omega $$ ω and the scalar field ( $$\phi $$ ϕ ) profile, expectedly, distinguishes between different solutions. Choosing specific localised forms for the free metric functions $$H'(u)$$ H ′ ( u ) (related to the wave profile) and J(u) (the gyraton) we obtain displacement memory effects using both geodesics and geodesic deviation. An interesting and easy-to-understand exactly solvable case arises when $$\omega =-2$$ ω = - 2 (with J(u) absent) which we discuss in detail. For other $$\omega $$ ω (in the presence of J or without), numerically obtained geodesics lead to results on displacement memory which appear to match qualitatively with those found from a deviation analysis. Thus, the issue of how memory effects in BD theory may arise and also differ from their GR counterparts, is now partially addressed, at least theoretically, within the context of this new class of Kundt geometries.
url https://doi.org/10.1140/epjc/s10052-021-09118-4
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