2017
DOI: 10.1103/physrevd.95.044045
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Gravitational waves and mass ejecta from binary neutron star mergers: Effect of the stars’ rotation

Abstract: We present new (3+1) dimensional numerical relativity simulations of the binary neutron star (BNS) mergers that take into account the NS spins. We consider different spin configurations, aligned or antialigned to the orbital angular momentum, for equal and unequal mass BNS and for two equations of state. All the simulations employ quasiequilibrium circular initial data in the constant rotational velocity approach, i.e. they are consistent with Einstein equations and in hydrodynamical equilibrium. We study the … Show more

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Cited by 124 publications
(163 citation statements)
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“…It is important to point out that for similar resolutions, cf. [70,71], the dephasing and consequently the shift in the merger time between similar resolutions have been significantly smaller for EoSs without phase transition. The bottom panel of Fig.…”
Section: The Inspiralmentioning
confidence: 92%
“…It is important to point out that for similar resolutions, cf. [70,71], the dephasing and consequently the shift in the merger time between similar resolutions have been significantly smaller for EoSs without phase transition. The bottom panel of Fig.…”
Section: The Inspiralmentioning
confidence: 92%
“…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%