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Optimising gravitational waves follow-up using galaxies stellar mass

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 Publication date 2019
  fields Physics
and research's language is English




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We present a new strategy to optimise the electromagnetic follow-up of gravitational wave triggers. This method is based on the widely used galaxy targeting approach where we add the stellar mass of galaxies in order to prioritise the more massive galaxies. We crossmatched the GLADE galaxy catalog with the AllWISE catalog up to 400Mpc with an efficiency of $sim$93%, and derived stellar masses using a stellar-to-mass ratio using the WISE1 band luminosity. We developed a new grade to rank galaxies combining their 3D localisation probability associated to the gravitational wave event with the new stellar mass information. The efficiency of this new approach is illustrated with the GW170817 event, which shows that its host galaxy, NGC4993, is ranked at the first place using this new method. The catalog, named Mangrove, is publicly available and the ranking of galaxies is automatically provided through a dedicated web site for each gravitational wave event.



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137 - M. Branchesi 2012
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Obtaining a better understanding of intermediate-mass black holes (IMBHs) is crucial, as their properties could shed light on the origin and growth of their supermassive counterparts. Massive star-forming clumps, which are present in a large fraction of massive galaxies at $z sim$ 1-3, are amongst the venues wherein IMBHs could reside. We perform a series of Fokker-Planck simulations to explore the occurrence of tidal disruption (TD) and gravitational wave (GW) events about an IMBH in a massive star-forming clump, modelling the latter so that its mass ($10^8 ,{rm M}_{odot}$) and effective radius ($100$ pc) are consistent with the properties of both observed and simulated clumps. We find that the TD and GW event rates are in the ranges $10^{-6}$-$10^{-5}$ and $10^{-8}$-$10^{-7}$ yr$^{-1}$, respectively, depending on the assumptions for the initial inner density profile of the system ($rho propto r^{-2}$ or $propto r^{-1}$) and the initial mass of the central IMBH ($10^5$ or $10^3,{rm M}_{odot}$). By integrating the GW event rate over $z$ = 1-3, we expect that the Laser Interferometer Space Antenna will be able to detect $sim$2 GW events per yr coming from these massive clumps; the intrinsic rate of TD events from these systems amounts instead to a few $10^3$ per yr, a fraction of which will be observable by, e.g. the Square Kilometre Array and the Advanced Telescope for High Energy Astrophysics. In conclusion, our results support the idea that the forthcoming GW and electromagnetic facilities may have the unprecedented opportunity of unveiling the lurking population of IMBHs.
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