Abstract

For third generation gravitational wave detectors, such as the Einstein Telescope, gravitational wave signals from binary neutron stars can last up to a few days before the neutron stars merge. To estimate the measurement uncertainties of key signal parameters, we develop a Fisher matrix approach which accounts for effects on such long duration signals of the time-dependent detector response and the earths rotation. We use this approach to characterize the sky localization uncertainty for gravitational waves from binary neutron stars at 40, 200, 400, 800 and 1600Mpc, for the Einstein Telescope and Cosmic Explorer individually and operating as a network. We find that the Einstein Telescope alone can localize the majority of detectable binary neutron stars at a distance of $\leq200$Mpc to within $100\text{deg}^2$ with 90% confidence. A network consisting of the Einstein Telescope and Cosmic Explorer can enhance the sky localization performance significantly - with the 90% credible region of $\mathcal{O}(1) \text{deg}^2$ for most sources at $\leq200$Mpc and $\leq100\text{deg}^2$ for most sources at $\leq1600$Mpc. We also investigate the prospects for third generation detectors identifying the presence of a signal prior to merger. To do this, we require a signal to have a network signal-to-noise ratio of $\geq12$ and $\geq5.5$ for at least two interferometers, and to have a 90% credible region for the sky localization that is no larger than $100 \text{deg}^2$. We find that the Einstein Telescope can send out such "early-warning" detection alerts 1 - 20 hours before merger for 100% of detectable binary neutron stars at 40Mpc and for $\sim58\%$ of sources at 200Mpc. For sources at a distance of 400Mpc, a network of the Einstein telescope and Cosmic Explorer can produce detection alerts up to $\sim 3$ hours prior to merger for 98% of detectable binary neutron stars.

Highlights

  • The first detections of gravitational waves (GWs) from binary black hole (BBH) systems GW150914, GW151226, GW170104, and GW170608 by the two LIGO detectors at Hanford and Livingston [1,2,3,4] have opened a new window on the universe and marked the beginning of gravitational wave (GW) astronomy

  • The time at the detector is denoted by t which is equal to the arrival time t0 of the incoming wave at the center of the earth, plus the time τ required for the wave to travel from the center of the earth to the detector, given by τ n· c r where n is the GW propagation direction and r is the location vector of the detector relative to the center of the

  • For a network with only one interferometer, namely, Cosmic Explorer (CE), we require that the accumulated signal to noise ratio (SNR) is no less than 12 to claim a detection

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Summary

Introduction

The first detections of gravitational waves (GWs) from binary black hole (BBH) systems GW150914, GW151226, GW170104, and GW170608 by the two LIGO detectors at Hanford and Livingston [1,2,3,4] have opened a new window on the universe and marked the beginning of gravitational wave (GW) astronomy. In 2017, VIRGO began observation and the first joint detection GW170814 was made by LIGO and VIRGO together [5]. Just a few days later, the three GW observatories detected the first binary neutron star (BNS) merger event GW170817 [6]. The detections of multiple electromagnetic (EM) counterparts associated with GW170817 initiated the era of GW multi-messenger astronomy [7,8,9,10,11].

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