{"title":"Follow-up of Neutron Star Mergers with CTA and Prospects for Joint Detection with Gravitational-Wave Detectors","authors":"T. Mondal, S. Chakraborty, L. Resmi, D. Bose","doi":"arxiv-2409.07916","DOIUrl":null,"url":null,"abstract":"The joint gravitational wave (GW) and electromagnetic observations of the\nbinary neutron star (BNS) merger GW170817 marked a giant leap in\nmulti-messenger astrophysics. The extensive observation campaign of the\nassociated Gamma-Ray Burst (GRB) and its afterglow has strengthened the\nhypothesis associating GRBs with BNS mergers and provided insights on mass\nejection, particularly the relativistic outflow launched in BNS mergers. In\nthis paper, we investigate the joint detection probabilities of BNS mergers by\nGW detectors and the upcoming ground-based very-high-energy (VHE) $\\gamma$-ray\ninstrument, the Cherenkov Telescope Array (CTA). Using an empirical relation\nthat constrains the distance-inclination angle plane, we simulated BNS mergers\ndetectable in the O5 run of the LIGO/Virgo/Kagra (LVK) network with $300$~Mpc\nBNS horizon. Assuming Gaussian structured jets and ignoring large sky\nlocalization challenges of GW detectors, we estimated VHE afterglow detection\nprobability by CTA. We have explored the afterglow parameter space to identify\nconditions favourable for detecting synchrotron self-Compton emission by CTA.\nOur study reveals that events viewed at angles $\\lesssim3$ times the jet core\nangle are detectable by CTA when the initial bulk Lorentz factor at the jet\naxis ranges between 100 and 800. We find high kinetic energy ($E_k>10^{50}$\nerg), ambient density ($n_0>10^{-1}$ $cm^{-3}$), and energy content in\nnon-thermal electrons significantly enhance the likelihood of CTA detection\nwithin 300 Mpc. The joint detection rate varies significantly with afterglow\nparameter distributions, ranging from $0.003$ to $0.5$ per year.","PeriodicalId":501343,"journal":{"name":"arXiv - PHYS - High Energy Astrophysical Phenomena","volume":"5 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Astrophysical Phenomena","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.07916","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The joint gravitational wave (GW) and electromagnetic observations of the
binary neutron star (BNS) merger GW170817 marked a giant leap in
multi-messenger astrophysics. The extensive observation campaign of the
associated Gamma-Ray Burst (GRB) and its afterglow has strengthened the
hypothesis associating GRBs with BNS mergers and provided insights on mass
ejection, particularly the relativistic outflow launched in BNS mergers. In
this paper, we investigate the joint detection probabilities of BNS mergers by
GW detectors and the upcoming ground-based very-high-energy (VHE) $\gamma$-ray
instrument, the Cherenkov Telescope Array (CTA). Using an empirical relation
that constrains the distance-inclination angle plane, we simulated BNS mergers
detectable in the O5 run of the LIGO/Virgo/Kagra (LVK) network with $300$~Mpc
BNS horizon. Assuming Gaussian structured jets and ignoring large sky
localization challenges of GW detectors, we estimated VHE afterglow detection
probability by CTA. We have explored the afterglow parameter space to identify
conditions favourable for detecting synchrotron self-Compton emission by CTA.
Our study reveals that events viewed at angles $\lesssim3$ times the jet core
angle are detectable by CTA when the initial bulk Lorentz factor at the jet
axis ranges between 100 and 800. We find high kinetic energy ($E_k>10^{50}$
erg), ambient density ($n_0>10^{-1}$ $cm^{-3}$), and energy content in
non-thermal electrons significantly enhance the likelihood of CTA detection
within 300 Mpc. The joint detection rate varies significantly with afterglow
parameter distributions, ranging from $0.003$ to $0.5$ per year.