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Article: A More Stringent Constraint on the Mass Ratio of Binary Neutron Star Merger GW170817

TitleA More Stringent Constraint on the Mass Ratio of Binary Neutron Star Merger GW170817
Authors
Keywordsgravitational waves
Issue Date2017
Citation
Astrophysical Journal Letters, 2017, v. 851, n. 2, article no. L45 How to Cite?
AbstractRecently, the LIGO-Virgo Collaborations reported their first detection of gravitational-wave (GW) signals from the low-mass compact binary merger GW170817, which is most likely due to a double neutron star (NS) merger. With the GW signals only, the chirp mass of the binary is precisely constrained to 1.188-0.002+0.004 M, but the mass ratio is loosely constrained in the range 0.4-1, so that a very rough estimation of the individual NS masses (1.36M 1 < 2.26M and 0.86M < M2 < 1.36M) was obtained. Here, we propose that if one can constrain the dynamical ejecta mass through performing kilonova modeling of the optical/IR data, by utilizing an empirical relation between the dynamical ejecta mass and the mass ratio of NS binaries, one may place a more stringent constraint on the mass ratio of the system. For instance, considering that the red "kilonova" component is powered by the dynamical ejecta, we reach a tight constraint on the mass ratio in the range of 0.46-0.59. Alternatively, if the blue "kilonova" component is powered by the dynamical ejecta, the mass ratio would be constrained in the range of 0.53-0.67. Overall, such a multi-messenger approach could narrow down the mass ratio of GW170817 system to the range of 0.46-0.67, which gives a more precise estimation of the individual NS mass than pure GW signal analysis, i.e., 1.61 M < M1 < 2.11 M and 0.90 M < M2 < 1.16 M.
Persistent Identifierhttp://hdl.handle.net/10722/361409
ISSN
2023 Impact Factor: 8.8
2023 SCImago Journal Rankings: 2.766

 

DC FieldValueLanguage
dc.contributor.authorGao, He-
dc.contributor.authorCao, Zhoujian-
dc.contributor.authorAi, Shunke-
dc.contributor.authorZhang, Bing-
dc.date.accessioned2025-09-16T04:16:45Z-
dc.date.available2025-09-16T04:16:45Z-
dc.date.issued2017-
dc.identifier.citationAstrophysical Journal Letters, 2017, v. 851, n. 2, article no. L45-
dc.identifier.issn2041-8205-
dc.identifier.urihttp://hdl.handle.net/10722/361409-
dc.description.abstractRecently, the LIGO-Virgo Collaborations reported their first detection of gravitational-wave (GW) signals from the low-mass compact binary merger GW170817, which is most likely due to a double neutron star (NS) merger. With the GW signals only, the chirp mass of the binary is precisely constrained to 1.188-0.002+0.004 M<inf>⊙</inf>, but the mass ratio is loosely constrained in the range 0.4-1, so that a very rough estimation of the individual NS masses (1.36M<inf>⊙</inf> <M<inf>1</inf> < 2.26M<inf>⊙</inf> and 0.86M<inf>⊙</inf> < M<inf>2</inf> < 1.36M<inf>⊙</inf>) was obtained. Here, we propose that if one can constrain the dynamical ejecta mass through performing kilonova modeling of the optical/IR data, by utilizing an empirical relation between the dynamical ejecta mass and the mass ratio of NS binaries, one may place a more stringent constraint on the mass ratio of the system. For instance, considering that the red "kilonova" component is powered by the dynamical ejecta, we reach a tight constraint on the mass ratio in the range of 0.46-0.59. Alternatively, if the blue "kilonova" component is powered by the dynamical ejecta, the mass ratio would be constrained in the range of 0.53-0.67. Overall, such a multi-messenger approach could narrow down the mass ratio of GW170817 system to the range of 0.46-0.67, which gives a more precise estimation of the individual NS mass than pure GW signal analysis, i.e., 1.61 M<inf>⊙</inf> < M<inf>1</inf> < 2.11 M<inf>⊙</inf> and 0.90 M<inf>⊙</inf> < M<inf>2</inf> < 1.16 M<inf>⊙</inf>.-
dc.languageeng-
dc.relation.ispartofAstrophysical Journal Letters-
dc.subjectgravitational waves-
dc.titleA More Stringent Constraint on the Mass Ratio of Binary Neutron Star Merger GW170817-
dc.typeArticle-
dc.description.naturelink_to_subscribed_fulltext-
dc.identifier.doi10.3847/2041-8213/aaa0c6-
dc.identifier.scopuseid_2-s2.0-85039715327-
dc.identifier.volume851-
dc.identifier.issue2-
dc.identifier.spagearticle no. L45-
dc.identifier.epagearticle no. L45-
dc.identifier.eissn2041-8213-

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