Abstract

Abstract Current and future optical and near-infrared wide-field surveys have the potential to find kilonovae, the optical and infrared counterparts to neutron star mergers, independently of gravitational-wave or high-energy gamma-ray burst triggers. The ability to discover fast and faint transients such as kilonovae largely depends on the area observed, the depth of those observations, the number of revisits per field in a given time frame, and the filters adopted by the survey; it also depends on the ability to perform rapid follow-up observations to confirm the nature of the transients. In this work, we assess kilonova detectability in existing simulations of the Legacy Survey of Space and Time strategy for the Vera C. Rubin Wide Fast Deep survey, with focus on comparing rolling to baseline cadences. Although currently available cadences can enable the detection of >300 kilonovae out to ∼1400 Mpc over the 10 year survey, we can expect only 3–32 kilonovae similar to GW170817 to be recognizable as fast-evolving transients. We also explore the detectability of kilonovae over the plausible parameter space, focusing on viewing angle and ejecta masses. We find that observations in redder izy bands are crucial for identification of nearby (within 300 Mpc) kilonovae that could be spectroscopically classified more easily than more distant sources. Rubin’s potential for serendipitous kilonova discovery could be increased by gain of efficiency with the employment of individual 30 s exposures (as opposed to 2 × 15 s snap pairs), with the addition of red-band observations coupled with same-night observations in g or r bands, and possibly with further development of a new rolling-cadence strategy.

Highlights

  • Binary neutron star (BNS) and neutron star–black hole (NSBH) mergers have long been predicted to be associated with short gamma-ray bursts (GRBs; e.g., andreoni@caltech.eduBlinnikov et al 1984), and optical/infrared transients called kilonovae (e.g., Li & Paczynski 1998)

  • Rates of BNS mergers are still highly uncertain, with R = 80 − 810 Gpc−3 yr−1 based on GW observations (The LIGO Scientific Collaboration et al 2020); empirical limits on kilonovae rates by optical surveys are nearing the upper end of the gravitational-wave measurements (Andreoni et al 2020; Andreoni & Coughlin et al 2021)

  • We found that rolling cadences, in which a smaller fraction of the footprint is observed in each season at higher cadence, perform significantly (∼ 50 − 60%) worse as coded for the v1.7 release than the baseline cadence8

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Summary

Introduction

Dynamical ejecta (e.g., Hotokezaka et al 2013; Bauswein et al 2013; Dietrich & Ujevic 2017), which arise from tidal stripping of the neutron star(s) and the neutron stars contact interface, and post-merger ejecta (e.g., Metzger et al 2008; Fernandez et al 2015; Siegel & Metzger 2018; Fernandez et al 2019), which arise from accretion disk winds surrounding the remnant object, are characterized by low electron fractions This scenario favors the production of heavy elements such as lanthanides and actinides via rapid neutron capture (known as the r-process), and the decay of these unstable nuclei powers the optical/infrared kilonova (e.g., Lattimer & Schramm 1974; Kasen et al 2013; Barnes & Kasen 2013; Barnes et al 2016; Kasen et al 2017).

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