2017
DOI: 10.1103/physrevd.95.024029
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Gravitational waves and mass ejecta from binary neutron star mergers: Effect of the mass ratio

Abstract: We present new (3+1)D numerical relativity simulations of the binary neutron star (BNS) merger and postmerger phase. We focus on a previously inaccessible region of the binary parameter space spanning the binary's mass-ratio q ∼ 1.00 − 1.75 for different total masses and equations of state, and up to q ∼ 2 for a stiff BNS system. We study the mass-ratio effect on the gravitational waves (GWs) and on the possible electromagnetic emission associated to dynamical mass ejecta. We compute waveforms, spectra, and sp… Show more

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Cited by 190 publications
(183 citation statements)
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“…Compared to the SLy simulations in Refs. [52,70] this is only about ∼ 15 to 40% of the SLy simulations. This means that if even half of the disk would be ejected (see Fig.…”
Section: Ejecta and Electromagnetic Counterpartsmentioning
confidence: 90%
“…Compared to the SLy simulations in Refs. [52,70] this is only about ∼ 15 to 40% of the SLy simulations. This means that if even half of the disk would be ejected (see Fig.…”
Section: Ejecta and Electromagnetic Counterpartsmentioning
confidence: 90%
“…Two coupling frequencies are identified from secondary peaks of the spectra, see e.g. [21,22,73,74] (and figures below in this paper); we indicate them asf 2±0 following the notation of [24]. Although we will often refer to discrete frequencies (spectral peaks), we stress that the GW frequency is not constant but evolves (chirp-like) as the remnant becomes more compact and eventually collapses (see SLy data in Fig.…”
Section: Nrpm Modelmentioning
confidence: 99%
“…KiloHertz GWs contain the imprint of the merger remnant dynamics. The main signature is a short GW transient peaking at a few characteristic frequencies, the dominant one being associated with twice the rotation frequency of the remnant NS at f 2 > f mrg [16,[21][22][23][24][25][26][27][28][29][30]. The transient is more luminous for short-lived remnant than for longlived; an absolute upper limit to the energy per unit mass is 0.126( M 2.8M ) M c 2 , where M is the binary mass [12].…”
Section: Introductionmentioning
confidence: 99%
“…For example, short-lived hypermassive NSs are expected to emit a few percent of a solar mass in GW energy (e.g., see the two lower dashed lines in Figure 1 that represent 1% and 10% of a solar mass; Kiuchi et al 2009;Clark et al 2014;Bernuzzi et al 2015b;Endrizzi et al 2016;Dietrich et al 2017aDietrich et al , 2017bFeo et al 2017), while our minimum 50% efficiency is   E M c 4.8 Corsi & Mészáros 2009). Figure 1 shows the h rss 50% for the considered waveform models as a function of the waveform's signal-weighted frequency.…”
Section: Implications and Conclusionmentioning
confidence: 99%