2016
DOI: 10.1103/physrevlett.116.181101
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Effects of Neutron-Star Dynamic Tides on Gravitational Waveforms within the Effective-One-Body Approach

Abstract: Extracting the unique information on ultradense nuclear matter from the gravitational waves emitted by merging neutron-star binaries requires robust theoretical models of the signal. We develop a novel effective-one-body waveform model that includes, for the first time, dynamic (instead of only adiabatic) tides of the neutron star as well as the merger signal for neutron-star-black-hole binaries. We demonstrate the importance of the dynamic tides by comparing our model against new numerical-relativity simulati… Show more

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Cited by 271 publications
(321 citation statements)
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“…The basic observation is that, when tidal deformabilities are included in a waveform model in a reasonable way, one can expect the ambiguity in relating back to the equation of state to be a single number that can be measured by fitting the model to a binary black hole waveform. More traditional semi-analytic methods (e.g., [33][34][35][36]) rely on numerical simulations of neutron star mergers for calibration. The method proposed here calibrates with vacuum (black hole) simulations, which are computationally cheaper and hence more practical to perform in the challenging early-inspiral regime.…”
Section: The Waveformmentioning
confidence: 99%
“…The basic observation is that, when tidal deformabilities are included in a waveform model in a reasonable way, one can expect the ambiguity in relating back to the equation of state to be a single number that can be measured by fitting the model to a binary black hole waveform. More traditional semi-analytic methods (e.g., [33][34][35][36]) rely on numerical simulations of neutron star mergers for calibration. The method proposed here calibrates with vacuum (black hole) simulations, which are computationally cheaper and hence more practical to perform in the challenging early-inspiral regime.…”
Section: The Waveformmentioning
confidence: 99%
“…In addition, the GW of BNS is almost entirely determined by the mass ratio q and the κ T 2 , because the binary total mass scales trivially in absence of tides and its de- pendency in the tidal waveform is hidden in the κ T 2 . Although other tidal polarizability parameters, corresponding to higher-than-quadrupole interactions, do play a role in the detailed modeling of the GW [69][70][71], the leading order κ T 2 encodes the main effect and it is the only tidal parameter measurable in GW searches. The coverage of the q-κ T 2 parameter space by our simulations is shown in Fig.…”
Section: Bns Configurationsmentioning
confidence: 99%
“…These include studies of the linear equilibrium tide [12,21,23,28,32,44] and the linear dynamical tide in non-rotating NSs [29,33,46,49,61] and rotating NSs [27,30,34]. The equilibrium and dynamical tide refer, respectively, to the quasi-static and resonant response of a star to a tidal field (see, e.g., [41]).…”
Section: Introductionmentioning
confidence: 99%