30 research outputs found
Open data from the third observing run of LIGO, Virgo, KAGRA, and GEO
- Author
- Abbott R.
- Abe H.
- Acernese F.
- Ackley K.
- Adhicary S.
- Adhikari N.
- Adhikari R.X.
- Adkins V.K.
- Adya V.B.
- Affeldt C.
- Agarwal D.
- Agathos M.
- Aguiar O.D.
- Aiello L.
- Ain A.
- Ajith P.
- Akutsu T.
- Al-Jodah A.
- Albanesi S.
- Alfaidi R.A.
- Allocca A.
- Alléné C.
- Almualla M.
- Altin P.A.
- Amato A.
- Amez-Droz L.
- Amorosi A.
- Anand S.
- Ananyeva A.
- Andersen R.
- Anderson S.B.
- Anderson W.G.
- Andia M.
- Ando M.
- Andrade T.
- Andres N.
- Andrić T.
- Andrés-Carcasona M.
- Ansoldi S.
- Antelis J.M.
- Antier S.
- Aoumi M.
- Apostolatos T.
- Appavuravther E.Z.
- Appert S.
- Apple S.K.
- Arai K.
- Araya A.
- Araya M.C.
- Areeda J.S.
- Aritomi N.
- Arnaud N.
- Arogeti M.
- Aronson S.M.
- Arun K.G.
- Arène M.
- Asada H.
- Ashton G.
- Aso Y.
- Assiduo M.
- Assis de Souza Melo S.
- Aston S.M.
- Astone P.
- Aubin F.
- AultONeal K.
- Babak S.
- Badalyan A.
- Badaracco F.
- Badger C.
- Bae S.
- Bagnasco S.
- Bai Y.
- Baier J.G.
- Baiotti L.
- Baird J.
- Bajpai R.
- Baka T.
- Ball M.
- Ballardin G.
- Ballmer S.W.
- Baltus G.
- Banagiri S.
- Banerjee B.
- Bankar D.
- Baral P.
- Barayoga J.C.
- Barber J.
- Barish B.C.
- Barker D.
- Barneo P.
- Barone F.
- Barr B.
- Barsotti L.
- Barsuglia M.
- Barta D.
- Barthelmy S.D.
- Barton M.A.
- Bartos I.
- Basak S.
- Basalaev A.
- Bassiri R.
- Basti A.
- Bawaj M.
- Bayley J.C.
- Baylor A.C.
- Bazzan M.
- Bedakihale V.M.
- Beirnaert F.
- Bejger M.
- Bell A.S.
- Ben Yaala M.
- Benedetto V.
- Beniwal D.
- Benoit W.
- Bentley J.D.
- Bera S.
- Berbel M.
- Bergamin F.
- Berger B.K.
- Bernuzzi S.
- Beroiz M.
- Berry C.P.L.
- Bersanetti D.
- Bertolini A.
- Betzwieser J.
- Beveridge D.
- Bevins N.
- Bhandare R.
- Bhandari A.V.
- Bhardwaj U.
- Bhatt R.
- Bhattacharjee D.
- Bhaumik S.
- Bianchi A.
- Bilenko I.A.
- Bilicki M.
- Billingsley G.
- Bini S.
- Birnholtz O.
- Biscans S.
- Bischi M.
- Biscoveanu S.
- Bisht A.
- Biswas B.
- Bitossi M.
- Bizouard M.-A.
- Blackburn J.K.
- Blair C.D.
- Blair D.G.
- Blair R.M.
- Bobba F.
- Bode N.
- Bogaert G.
- Boileau G.
- Boldrini M.
- Bolingbroke G.N.
- Bonavena L.D.
- Bondarescu R.
- Bondu F.
- Bonilla E.
- Bonilla G.S.
- Bonnand R.
- Booker P.
- Bork R.
- Boschi V.
- Bose N.
- Bose S.
- Bossilkov V.
- Boudart Vincent
- Bouffanais Y.
- Bozzi A.
- Boër M.
- Bradaschia C.
- Brady P.R.
- Braglia M.
- Branch A.
- Branchesi M.
- Brau J.E.
- Breschi M.
- Briant T.
- Brillet A.
- Brinkmann M.
- Brockill P.
- Brooks A.F.
- Brooks J.
- Brown D.D.
- Brunett S.
- Bruno G.
- Bruntz R.
- Bryant J.
- Bucci F.
- Buchanan J.
- Bulashenko O.
- Bulik T.
- Bulten H.J.
- Buonanno A.
- Burtnyk K.
- Buscicchio R.
- Buskulic D.
- Buy C.
- Byer R.L.
- Bécsy B.
- Cabourn Davies G.S.
- Cabras G.
- Cabrita R.
- Cadonati L.
- Caesar S.
- Cagnoli G.
- Cahillane C.
- Calderón Bustillo J.
- Callaghan J.D.
- Callister T.A.
- Calloni E.
- Camp J.B.
- Canepa M.
- Caneva Santoro G.
- Cannavacciuolo M.
- Cannon K.C.
- Cao H.
- Cao Z.
- Capistran L.A.
- Capocasa E.
- Capote E.
- Carapella G.
- Carbognani F.
- Carlassara M.
- Carlin J.B.
- Carpinelli M.
- Carter J.J.
- Carullo G.
- Casanueva Diaz J.
- Casentini C.
- Castaldi G.
- Castro-Lucas S.Y.
- Caudill S.
- Cavaglià M.
- Cavalieri R.
- Cella G.
- Cerdá-Durán P.
- Cesarini E.
- Chaibi W.
- Chakalis W.
- Chalathadka Subrahmanya S.
- Champion E.
- Chan C.
- Chan C.L.
- Chandra K.
- Chang I.P.
- Chang W.
- Chanial P.
- Chao S.
- Chapman-Bird C.
- Charlton E.L.
- Charlton P.
- Chassande-Mottin E.
- Chastain L.
- Chatterjee C.
- Chatterjee Debarati
- Chatterjee Deep
- Chaturvedi M.
- Chaty S.
- Chatziioannou K.
- Chen D.
- Chen H.
- Chen H.Y.
- Chen J.
- Chen K.H.
- Chen X.
- Chen Y.
- Chen Y.-R.
- Cheng H.
- Chessa P.
- Cheung H.Y.
- Chia H.Y.
- Chiadini F.
- Chiang C.
- Chiang C.-I.
- Chiarini G.
- Chiba A.
- Chiba R.
- Chierici R.
- Chincarini A.
- Chiofalo M.L.
- Chiummo A.
- Choudhary S.
- Christensen N.
- Chua S.S.Y.
- Chung K.W.
- Ciani G.
- Ciecielag P.
- Cieślar M.
- Cifaldi M.
- Ciobanu A.A.
- Ciolfi R.
- Clara F.
- Clark J.A.
- Clarke T.A.
- Clearwater P.
- Clesse S.
- Cleva F.
- Coccia E.
- Codazzo E.
- Cohadon P.-F.
- Colleoni M.
- Collette Christophe
- Colombo A.
- Colpi M.
- Compton C.M.
- Conti L.
- Cooper S.J.
- Corban P.
- Corbitt T.R.
- Cordero-Carrión I.
- Corezzi S.
- Cornish N.J.
- Corsi A.
- Cortese S.
- Coschizza A.C.
- Cottingham R.
- Coughlin M.W.
- Coulon J.-P.
- Countryman S.T.
- Coupechoux J.-F.
- Cousins B.
- Couvares P.
- Coward D.M.
- Cowart M.J.
- Cowburn B.D.
- Coyne D.C.
- Coyne R.
- Craig K.
- Creighton J.D.E.
- Creighton T.D.
- Criswell A.W.
- Crockett-Gray J.C.G.
- Croquette M.
- Crowder S.G.
- Cudell Jean-René
- Cullen T.J.
- Cumming A.
- Cummings R.
- Cuoco E.
- Curyło M.
- D'Angelo B.
- D'Antonio S.
- D'Emilio V.
- D'Onofrio L.
- D'Urso D.
- Dabadie P.
- Dal Canton T.
- Dall'Osso S.
- Danilishin S.
- Danzmann K.
- Darroch K.E.
- Darsow-Fromm C.
- Dasgupta A.
- Datrier L.E.H.
- Datta Sayantani
- Dattilo V.
- Dave I.
- Davenport A.
- Davier M.
- Davis D.
- Davis M.C.
- Daw E.J.
- Dax M.
- De Laurentis M.
- De Lillo F.
- De Lillo N.
- De Matteis F.
- De Pietri R.
- De Rosa R.
- De Rossi C.
- De Simone R.
- DeBra D.
- Deenadayalan M.
- Degallaix J.
- Del Favero V.
- Del Pozzo W.
- Dell'Aquila D.
- Deléglise S.
- Demos N.
- Dent T.
- Depasse A.
- DeSalvo R.
- Dhurandhar S.
- Di Fiore L.
- Di Fronzo C.
- Di Giorgio C.
- Di Giovanni F.
- Di Giovanni M.
- Di Girolamo T.
- Di Lieto A.
- Di Michele A.
- Di Pace S.
- Di Palma I.
- Di Renzo F.
- Diab R.
- Diamond P.Z.
- Didio N.A.
- Dietrich T.
- Diksha D.
- Divyajyoti
- Dmitriev A.
- Doctor Z.
- Dohmen E.
- Doleva P.P.
- Donahue L.
- Donovan F.
- Dooley K.L.
- Dooney T.
- Doravari S.
- Dorosh O.
- Drago M.
- Driggers J.C.
- Drori Y.
- Ducoin J.-G.
- Dunn L.
- Dupletsa U.
- Durante O.
- Duverne P.-A.
- Dwyer S.E.
- Dálya G.
- Díaz M.C.
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- Easter P.J.
- Ebersold M.
- Eckhardt T.
- Eddolls G.
- Edelman B.
- Edo T.B.
- Edy O.
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- Eichholz J.
- Eisenmann M.
- Eisenstein R.A.
- Ejlli A.
- Engelby E.
- Engl A.J.
- Errico L.
- Essick R.C.
- Estellés H.
- Estevez D.
- Etzel T.
- Evans C.
- Evans M.
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- Evstafyeva T.
- Ewing B.E.
- Fabrizi F.
- Faedi F.
- Fafone V.
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- Fairhurst S.
- Fan P.C.
- Fan X.
- Farah A.M.
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- Farr W.M.
- Fauchon-Jones E.J.
- Favaro G.
- Favata M.
- Fays Maxime
- Feicht J.
- Fejer M.M.
- Fenyvesi E.
- Ferguson D.L.
- Fernandez-Galiana A.
- Ferrante I.
- Ferreira T.A.
- Fidecaro F.
- Figura P.
- Fiori A.
- Fiori I.
- Fishbach M.
- Fisher R.P.
- Fittipaldi R.
- Fiumara V.
- Flaminio R.
- Fleischer S.M.
- Fleming L.S.
- Floden E.
- Fong H.K.
- Font J.A.
- Fornal B.
- Forsyth P.W.F.
- Franke A.
- Frasca S.
- Frasconi F.
- Freed J.P.
- Frei Z.
- Freise A.
- Freitas O.
- Frey R.
- Fritschel P.
- Frolov V.V.
- Fronzé G.G.
- Fujimoto Y.
- Fukunaga I.
- Fulda P.
- Fyffe M.
- Gabbard H.A.
- Gabella W.E.
- Gadre B.U.
- Gaglani K.
- Gair J.R.
- Gais J.
- Galaudage S.
- Gallardo S.
- Gamba R.
- Ganapathy D.
- Ganguly A.
- Gao D.
- Gaonkar S.G.
- Garaventa B.
- Garcia-Bellido J.
- García-Núñez C.
- García-Quirós C.
- Gardner K.A.
- Gargiulo J.
- Garufi F.
- Gasbarra C.
- Gateley B.
- Gayathri V.
- Gemme G.
- Gennai A.
- George J.
- Gerberding O.
- Gergely L.
- Ghonge S.
- Ghosh Abhirup
- Ghosh Archisman
- Ghosh Shaon
- Ghosh Shrobana
- Ghosh T.
- Giacoppo L.
- Giaime J.A.
- Giardina K.D.
- Gibson D.R.
- Gier C.
- Giri P.
- Gissi F.
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- Glanzer J.
- Gleckl A.E.
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- Godfrey J.
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- Goetz E.
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- Gosselin M.
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- Gretarsson A.M.
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- Grote H.
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- Guerra D.
- Guetta D.
- Guidi G.M.
- Guimaraes A.R.
- Gulati H.K.
- Gulminelli F.
- Gunny A.M.
- Guo H.
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- Gupta Anchal
- Gupta Anuradha
- Gupta Ish
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- Heinze J.
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- Publication venue
- American Astronomical Society
- Publication date
- 01/01/2023
- Field of study
The global network of gravitational-wave observatories now includes five detectors, namely LIGO Hanford, LIGO Livingston, Virgo, KAGRA, and GEO 600. These detectors collected data during their third observing run, O3, composed of three phases: O3a starting in 2019 April and lasting six months, O3b starting in 2019 November and lasting five months, and O3GK starting in 2020 April and lasting two weeks. In this paper we describe these data and various other science products that can be freely accessed through the Gravitational Wave Open Science Center at https://gwosc.org. The main data set, consisting of the gravitational-wave strain time series that contains the astrophysical signals, is released together with supporting data useful for their analysis and documentation, tutorials, as well as analysis software packages
Search for eccentric black hole coalescences during the third observing run of LIGO and Virgo
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- Álvarez-López S.
- Publication venue
- American Astronomical Society
- Publication date
- 01/10/2024
- Field of study
Despite the growing number of binary black hole coalescences confidently observed through gravitational waves so far, the astrophysical origin of these binaries remains uncertain. Orbital eccentricity is one of the clearest tracers of binary formation channels. Identifying binary eccentricity, however, remains challenging due to the limited availability of gravitational waveforms that include the effects of eccentricity. Here, we present observational results for a waveform-independent search sensitive to eccentric black hole coalescences, covering the third observing run (O3) of the LIGO and Virgo detectors. We identified no new high-significance candidates beyond those that have already been identified with searches focusing on quasi-circular binaries. We determine the sensitivity of our search to high-mass (total source-frame mass M > 70 M⊙) binaries covering eccentricities up to 0.3 at 15 Hz emitted gravitational-wave frequency, and use this to compare model predictions to search results. Assuming all detections are indeed quasi-circular, for our fiducial population model, we place a conservative upper limit for the merger rate density of high-mass binaries with eccentricities 0 < e ≤ 0.3 at 16.9 Gpc−3 yr−1 at the 90% confidence level
Search for Eccentric Black Hole Coalescences during the Third Observing Run of LIGO and Virgo
- Author
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- Abbott R
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- Washington N.Y
- Watada K
- Watarai D
- Wayt K.E
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- Xu V.A
- Yaala M. Ben
- Yadav N
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- Yamamoto T.S
- Yamamura S
- Yamazaki R
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- Yang L.-C
- Yang Y.-C
- Yang Yang
- Yang Yi
- Yap M.J
- Yarbrough Z
- Yeh S.-W
- Yelikar A.B
- Yeung S.M.C
- Yeung T.Y
- Yokoyama J
- Yokozawa T
- Yoo J
- Yu H
- Yuzurihara H
- Zadrożny A
- Zannelli A.J
- Zanolin M
- Zeeshan M
- Zelenova T
- Zendri J.-P
- Zevin M
- Zhang J
- Zhang L
- Zhang R
- Zhang T
- Zhang Ya
- Zhang Yanqi
- Zhao C
- Zhao Yue
- Zhao Yuhang
- Zheng Y
- Zhong H
- Zhou R
- Zhu Z.-H
- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Álvarez-López S
- Publication venue
- HAL CCSD
- Publication date
- 17/10/2023
- Field of study
International audienceDespite the growing number of confident binary black hole coalescences observed through gravitational waves so far, the astrophysical origin of these binaries remains uncertain. Orbital eccentricity is one of the clearest tracers of binary formation channels. Identifying binary eccentricity, however, remains challenging due to the limited availability of gravitational waveforms that include effects of eccentricity. Here, we present observational results for a waveform-independent search sensitive to eccentric black hole coalescences, covering the third observing run (O3) of the LIGO and Virgo detectors. We identified no new high-significance candidates beyond those that were already identified with searches focusing on quasi-circular binaries. We determine the sensitivity of our search to high-mass (total mass M>70M⊙) binaries covering eccentricities up to 0.3 at 15 Hz orbital frequency, and use this to compare model predictions to search results. Assuming all detections are indeed quasi-circular, for our fiducial population model, we place an upper limit for the merger rate density of high-mass binaries with eccentricities 0<e≤0.3 at 0.33 Gpc−3 yr−1 at 90% confidence level
Swift-BAT GUANO follow-up of gravitational-wave triggers in the third LIGO-Virgo-KAGRA observing run
- Author
- Abac A.G
- Abbott R
- Abe H
- Abouelfettouh I
- Acernese F
- Ackley K
- Adamcewicz C
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- Ambrosi Elena
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- Xu Y
- Yaala M. Ben
- Yadav N
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- Yamamoto K
- Yamamoto M
- Yamamoto T
- Yamamoto T.S
- Yamamura S
- Yamazaki R
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- Yang K.Z
- Yang L.-C
- Yang Y
- Yarbrough Z
- Yeh S.-W
- Yelikar A.B
- Yeung S.M.C
- Yin X
- Yokoyama J
- Yokozawa T
- Yoo J
- Yu H
- Yuzurihara H
- Zadrożny A
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- Zeeshan M
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- Zhang A.C
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- Zhao Yue
- Zhao Yuhang
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- Zhu Z.-H
- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 10/09/2024
- Field of study
International audienceWe present results from a search for X-ray/gamma-ray counterparts of gravitational-wave (GW) candidates from the third observing run (O3) of the LIGO-Virgo-KAGRA (LVK) network using the Swift Burst Alert Telescope (Swift-BAT). The search includes 636 GW candidates received in low latency, 86 of which have been confirmed by the offline analysis and included in the third cumulative Gravitational-Wave Transient Catalogs (GWTC-3). Targeted searches were carried out on the entire GW sample using the maximum--likelihood NITRATES pipeline on the BAT data made available via the GUANO infrastructure. We do not detect any significant electromagnetic emission that is temporally and spatially coincident with any of the GW candidates. We report flux upper limits in the 15-350 keV band as a function of sky position for all the catalog candidates. For GW candidates where the Swift-BAT false alarm rate is less than 10−3 Hz, we compute the GW--BAT joint false alarm rate. Finally, the derived Swift-BAT upper limits are used to infer constraints on the putative electromagnetic emission associated with binary black hole mergers
Swift-BAT GUANO follow-up of gravitational-wave triggers in the third LIGO-Virgo-KAGRA observing run
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- Yeh S.-W
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- Yeung S.M.C
- Yin X
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- Yokozawa T
- Yoo J
- Yu H
- Yuzurihara H
- Zadrożny A
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- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 10/09/2024
- Field of study
International audienceWe present results from a search for X-ray/gamma-ray counterparts of gravitational-wave (GW) candidates from the third observing run (O3) of the LIGO-Virgo-KAGRA (LVK) network using the Swift Burst Alert Telescope (Swift-BAT). The search includes 636 GW candidates received in low latency, 86 of which have been confirmed by the offline analysis and included in the third cumulative Gravitational-Wave Transient Catalogs (GWTC-3). Targeted searches were carried out on the entire GW sample using the maximum--likelihood NITRATES pipeline on the BAT data made available via the GUANO infrastructure. We do not detect any significant electromagnetic emission that is temporally and spatially coincident with any of the GW candidates. We report flux upper limits in the 15-350 keV band as a function of sky position for all the catalog candidates. For GW candidates where the Swift-BAT false alarm rate is less than 10−3 Hz, we compute the GW--BAT joint false alarm rate. Finally, the derived Swift-BAT upper limits are used to infer constraints on the putative electromagnetic emission associated with binary black hole mergers
Observation of Gravitational Waves from the Coalescence of a 2.5−4.5 M⊙ Compact Object and a Neutron Star
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- Yasui H
- Yeh S.-W
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- Yin X
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- Yokozawa T
- Yoo J
- Yu H
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- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeeshan M
- Zelenova T
- Zendri J.-P
- Zeoli M
- Zerrad M
- Zevin M
- Zhang A.C
- Zhang L
- Zhang R
- Zhang T
- Zhang Y
- Zhao C
- Zhao Yue
- Zhao Yuhang
- Zheng Y
- Zhong H
- Zhou R
- Zhu X.-J
- Zhu Z.-H
- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2024
- Field of study
International audienceWe report the observation of a coalescing compact binary with component masses 2.5−4.5 M⊙ and 1.2−2.0 M⊙ (all measurements quoted at the 90% credible level). The gravitational-wave signal GW230529_181500 was observed during the fourth observing run of the LIGO-Virgo-KAGRA detector network on 2023 May 29 by the LIGO Livingston Observatory. The primary component of the source has a mass less than 5 M⊙ at 99% credibility. We cannot definitively determine from gravitational-wave data alone whether either component of the source is a neutron star or a black hole. However, given existing estimates of the maximum neutron star mass, we find the most probable interpretation of the source to be the coalescence of a neutron star with a black hole that has a mass between the most massive neutron stars and the least massive black holes observed in the Galaxy. We estimate a merger rate density of 55−47+127 Gpc−3yr−1 for compact binary coalescences with properties similar to the source of GW230529_181500; assuming that the source is a neutron star-black hole merger, GW230529_181500-like sources constitute about 60% of the total merger rate inferred for neutron star-black hole coalescences. The discovery of this system implies an increase in the expected rate of neutron star-black hole mergers with electromagnetic counterparts and provides further evidence for compact objects existing within the purported lower mass gap
Swift-BAT GUANO follow-up of gravitational-wave triggers in the third LIGO-Virgo-KAGRA observing run
- Author
- Abac A.G
- Abbott R
- Abe H
- Abouelfettouh I
- Acernese F
- Ackley K
- Adamcewicz C
- Adhicary S
- Adhikari N
- Adhikari R.X
- Adkins V.K
- Adya V.B
- Affeldt C
- Agarwal D
- Agathos M
- Aguiar O.D
- Aguilar I
- Aiello L
- Ain A
- Akutsu T
- Al-Jodah A
- Al-Shammari S
- Albanesi S
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- Yarbrough Z
- Yeh S.-W
- Yelikar A.B
- Yeung S.M.C
- Yin X
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- Yokozawa T
- Yoo J
- Yu H
- Yuzurihara H
- Zadrożny A
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- Zeeshan M
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- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 10/09/2024
- Field of study
International audienceWe present results from a search for X-ray/gamma-ray counterparts of gravitational-wave (GW) candidates from the third observing run (O3) of the LIGO-Virgo-KAGRA (LVK) network using the Swift Burst Alert Telescope (Swift-BAT). The search includes 636 GW candidates received in low latency, 86 of which have been confirmed by the offline analysis and included in the third cumulative Gravitational-Wave Transient Catalogs (GWTC-3). Targeted searches were carried out on the entire GW sample using the maximum--likelihood NITRATES pipeline on the BAT data made available via the GUANO infrastructure. We do not detect any significant electromagnetic emission that is temporally and spatially coincident with any of the GW candidates. We report flux upper limits in the 15-350 keV band as a function of sky position for all the catalog candidates. For GW candidates where the Swift-BAT false alarm rate is less than 10−3 Hz, we compute the GW--BAT joint false alarm rate. Finally, the derived Swift-BAT upper limits are used to infer constraints on the putative electromagnetic emission associated with binary black hole mergers
Ultralight vector dark matter search using data from the KAGRA O3GK run
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- Wysocki D.M
- Xiao L
- Xu V.A
- Xu Y
- Yaala M. Ben
- Yadav N
- Yamamoto H
- Yamamoto K
- Yamamoto M
- Yamamoto T
- Yamamoto T.S
- Yamamura S
- Yamazaki R
- Yan S
- Yan T
- Yang F
- Yang F.W
- Yang K.Z
- Yang L.-C
- Yang Y
- Yarbrough Z
- Yeh S.-W
- Yelikar A.B
- Yeung S.M.C
- Yin X
- Yokoyama J
- Yokozawa T
- Yoo J
- Yu H
- Yuzurihara H
- Zadrożny A
- Zannelli A.J
- Zanolin M
- Zeeshan M
- Zelenova T
- Zendri J.-P
- Zeoli M
- Zerrad M
- Zevin M
- Zhang A.C
- Zhang J
- Zhang L
- Zhang R
- Zhang T
- Zhang Y
- Zhao C
- Zhao Yue
- Zhao Yuhang
- Zheng Y
- Zhong H
- Zhong S
- Zhou R
- Zhu Z.-H
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2024
- Field of study
International audienceAmong the various candidates for dark matter (DM), ultralight vector DM can be probed by laser interferometric gravitational wave detectors through the measurement of oscillating length changes in the arm cavities. In this context, KAGRA has a unique feature due to differing compositions of its mirrors, enhancing the signal of vector DM in the length change in the auxiliary channels. Here we present the result of a search for U(1)B−L gauge boson DM using the KAGRA data from auxiliary length channels during the first joint observation run together with GEO600. By applying our search pipeline, which takes into account the stochastic nature of ultralight DM, upper bounds on the coupling strength between the U(1)B−L gauge boson and ordinary matter are obtained for a range of DM masses. While our constraints are less stringent than those derived from previous experiments, this study demonstrates the applicability of our method to the lower-mass vector DM search, which is made difficult in this measurement by the short observation time compared to the auto-correlation time scale of DM
Search for Eccentric Black Hole Coalescences during the Third Observing Run of LIGO and Virgo
- Author
- Abac A.G
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adamcewicz C
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- Adhikari R.X
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- Yeh S.-W
- Yelikar A.B
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- Yeung T.Y
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- Yuzurihara H
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- Zhao Yuhang
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- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Álvarez-López S
- Publication venue
- HAL CCSD
- Publication date
- 17/10/2023
- Field of study
International audienceDespite the growing number of confident binary black hole coalescences observed through gravitational waves so far, the astrophysical origin of these binaries remains uncertain. Orbital eccentricity is one of the clearest tracers of binary formation channels. Identifying binary eccentricity, however, remains challenging due to the limited availability of gravitational waveforms that include effects of eccentricity. Here, we present observational results for a waveform-independent search sensitive to eccentric black hole coalescences, covering the third observing run (O3) of the LIGO and Virgo detectors. We identified no new high-significance candidates beyond those that were already identified with searches focusing on quasi-circular binaries. We determine the sensitivity of our search to high-mass (total mass M>70M⊙) binaries covering eccentricities up to 0.3 at 15 Hz orbital frequency, and use this to compare model predictions to search results. Assuming all detections are indeed quasi-circular, for our fiducial population model, we place an upper limit for the merger rate density of high-mass binaries with eccentricities 0<e≤0.3 at 0.33 Gpc−3 yr−1 at 90% confidence level
Search for Eccentric Black Hole Coalescences during the Third Observing Run of LIGO and Virgo
- Author
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- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adamcewicz C
- Adhicary S
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- Adhikari R.X
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- Schmitz S.J
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- Yaala M. Ben
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- Yamamoto T.S
- Yamamura S
- Yamazaki R
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- Yang L.-C
- Yang Y.-C
- Yang Yang
- Yang Yi
- Yap M.J
- Yarbrough Z
- Yeh S.-W
- Yelikar A.B
- Yeung S.M.C
- Yeung T.Y
- Yokoyama J
- Yokozawa T
- Yoo J
- Yu H
- Yuzurihara H
- Zadrożny A
- Zannelli A.J
- Zanolin M
- Zeeshan M
- Zelenova T
- Zendri J.-P
- Zevin M
- Zhang J
- Zhang L
- Zhang R
- Zhang T
- Zhang Ya
- Zhang Yanqi
- Zhao C
- Zhao Yue
- Zhao Yuhang
- Zheng Y
- Zhong H
- Zhou R
- Zhu Z.-H
- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Álvarez-López S
- Publication venue
- HAL CCSD
- Publication date
- 17/10/2023
- Field of study
International audienceDespite the growing number of confident binary black hole coalescences observed through gravitational waves so far, the astrophysical origin of these binaries remains uncertain. Orbital eccentricity is one of the clearest tracers of binary formation channels. Identifying binary eccentricity, however, remains challenging due to the limited availability of gravitational waveforms that include effects of eccentricity. Here, we present observational results for a waveform-independent search sensitive to eccentric black hole coalescences, covering the third observing run (O3) of the LIGO and Virgo detectors. We identified no new high-significance candidates beyond those that were already identified with searches focusing on quasi-circular binaries. We determine the sensitivity of our search to high-mass (total mass M>70M⊙) binaries covering eccentricities up to 0.3 at 15 Hz orbital frequency, and use this to compare model predictions to search results. Assuming all detections are indeed quasi-circular, for our fiducial population model, we place an upper limit for the merger rate density of high-mass binaries with eccentricities 0<e≤0.3 at 0.33 Gpc−3 yr−1 at 90% confidence level