@gpkulkarni

Galaxy fields of LISA massive black hole mergers in a simulated Universe

, , , , , and . (2022)cite arxiv:2207.10683Comment: 25 pages, 14 Figures, To be submitted to MNRAS.

Abstract

LISA will extend the search for gravitational waves (GWs) at $0.1\,-\,100$ mHz where loud signals from coalescing binary black holes of $ 10^4 \,-\,10^7\,M_ødot$ are expected. Depending on their mass and luminosity distance, the uncertainty in the LISA sky-localization decreases from hundreds of deg$^2$ during the inspiral phase to fractions of a deg$^2$ after the merger. By using the semi-analytical model L-Galaxies applied to the Millennium-I merger trees, we generate a simulated Universe to identify the hosts of $z\,łeq\,3$ coalescing binaries with total mass of $3\,\times\,10^5$, $3\,\times\,10^6$ and $3\,\times\,10^7\rm M_ødot$, and varying mass ratio. We find that, even at the time of merger, the number of galaxies around the LISA sources is too large ($\gtrsim\,10^2$) to allow direct host identification. However, if an X-ray counterpart is associated to the GW sources at $z\,<\,1$, all LISA fields at merger are populated by $łesssim\,10$ AGNs emitting above $\sim\, 10^-17 \, \rm erg\,cm^-2\,s^-1$. For sources at higher redshifts, the poorer sky-localization causes this number to increase up to $\sim\, 10^3$. Archival data from eRosita will allow discarding $\sim\, 10\%$ of these AGNs, being too shallow to detect the dim X-ray luminosity of the GW sources. Inspiralling binaries in an active phase with masses $łesssim\,10^6M_ødot$ at $z\,łeq\,0.3$ can be detected, as early as $10$ hours before the merger, by future X-ray observatories in less than a few minutes. For these systems, $łesssim\,10$ AGNs are within the LISA sky-localization area. Finally, the LISA-Taiji network would guarantee the identification of an X-ray counterpart $10$ hours before merger for all binaries at $z\,łesssim\,1$.

Description

Galaxy fields of LISA massive black hole mergers in a simulated Universe

Links and resources

Tags