2024MNRAS.527.4378K


Query : 2024MNRAS.527.4378K

2024MNRAS.527.4378K - Mon. Not. R. Astron. Soc., 527, 4378-4387 (2024/January-3)

Gertsenshtein-Zel'dovich effect: a plausible explanation for fast radio bursts?

KUSHWAHA A., MALIK S. and SHANKARANARAYANAN S.

Abstract (from CDS):

We present a novel model that may provide an interpretation for a class of non-repeating fast radio bursts (FRBs) - short ($\lt 1~\rm {s}$), bright ($0.1 - 1000~\rm {Jy}$) bursts of MHz-GHz frequency radio waves. The model has three ingredients - compact object, a progenitor with effective magnetic field strength around 1010 Gauss, and high-frequency (MHz-GHz) gravitational waves (GWs). At resonance, the energy conversion from GWs to electromagnetic waves occurs when GWs pass through the magnetosphere of such compact objects due to the Gertsenshtein-Zel'dovich effect. This conversion produces bursts of electromagnetic waves in the MHz-GHz range, leading to FRBs. Our model has three key features: (i) predict peak flux, (ii) can naturally explain the pulse width, and (iii) coherent nature of FRB. We thus conclude that the neutron star/magnetar could be the progenitor of FRBs. Further, our model offers a novel perspective on the indirection detection of GWs at high-frequency beyond detection capabilities. Thus, transient events like FRBs are a rich source for the current era of multi-messenger astronomy.

Abstract Copyright: © The Author(s) 2023. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): physical data and processes: gravitational waves - magnetic fields - methods: analytical - stars: neutron - pulsars: general - fast radio bursts: general

Simbad objects: 4

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Number of rows : 4
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 FRB 010125 rB 19 06 53.00 -40 37 14.4           ~ 46 1
2 NAME Sgr 1935+2154 * 19 34 55.68 +21 53 48.2           ~ 820 1
3 FRB 200428 rB 19 35.0 +21 57           ~ 291 0
4 FRB 120127 rB 23 15 06.0 -18 25 37           ~ 51 0

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