45 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.
- Arellano F.E.P.
- 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.
- 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 V.
- 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.
- 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 D.
- Chatterjee D.
- Chaturvedi M.
- Chaty S.
- Chatziioannou K.
- Chaudhary S.S.
- Chen D.
- Chen H.
- Chen H.Y.
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- 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 C.G.
- 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 J.R.
- Cullen T.J.
- Cumming A.
- Cummings R.
- Cuoco E.
- Curyło M.
- 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 S.
- 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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- D’Emilio V.
- D’Onofrio L.
- D’Urso D.
- e Melo I.T.
- Eassa C.
- Easter P.J.
- Ebersold M.
- Eckhardt T.
- Eddolls G.
- Edelman B.
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- Edy O.
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- 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.
- Evans T.M.
- Evstafyeva T.
- Ewing B.E.
- Fabrizi F.
- Faedi F.
- Fafone V.
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- Fairhurst S.
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- Fan X.
- Farah A.M.
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- Farr W.M.
- Fauchon-Jones E.J.
- Favaro G.
- Favata M.
- Fays M.
- 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 A.
- Ghosh A.
- Ghosh S.
- Ghosh S.
- Ghosh T.
- Giacoppo L.
- Giaime J.A.
- Giardina K.D.
- Gibson D.R.
- Gier C.
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- Glanzer J.
- Gleckl A.E.
- Glotin F.
- Godfrey J.
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- González G.
- Gosselin M.
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- Griggs H.L.
- Grignani G.
- Grimaldi A.
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- Guerra D.
- Guetta D.
- Guidi G.M.
- Guimaraes A.R.
- Gulati H.K.
- Gulminelli F.
- Gunny A.M.
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- Gutierrez N.
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- Himemoto Y.
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- Hsieh B.-H.
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- Zucker M.E.
- Zweizig J.
- Publication venue
- American Astronomical Society
- Publication date
- 01/01/2023
- Field of study
Get PDFThe 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 gravitational-wave transients associated with magnetar bursts in advanced LIGO and advanced Virgo data from the third observing run
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- Abbott R
- Abe H
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- Ying M
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- Publication venue
- American Astronomical Society
- Publication date
- 01/01/2024
- Field of study
Get PDFGravitational waves are expected to be produced from neutron star oscillations associated with magnetar giant f lares and short bursts. We present the results of a search for short-duration (milliseconds to seconds) and longduration (∼100 s) transient gravitational waves from 13 magnetar short bursts observed during Advanced LIGO, Advanced Virgo, and KAGRA’s third observation run. These 13 bursts come from two magnetars, SGR1935 +2154 and SwiftJ1818.0−1607. We also include three other electromagnetic burst events detected by FermiGBM which were identified as likely coming from one or more magnetars, but they have no association with a known magnetar. No magnetar giant flares were detected during the analysis period. We find no evidence of gravitational waves associated with any of these 16 bursts. We place upper limits on the rms of the integrated incident gravitational-wave strain that reach 3.6 × 10−²³ Hz at 100 Hz for the short-duration search and 1.1 ×10−²² Hz at 450 Hz for the long-duration search. For a ringdown signal at 1590 Hz targeted by the short-duration search the limit is set to 2.3 × 10−²² Hz. Using the estimated distance to each magnetar, we derive upper limits upper limits on the emitted gravitational-wave energy of 1.5 × 1044 erg (1.0 × 1044 erg) for SGR 1935+2154 and 9.4 × 10^43 erg (1.3 × 1044 erg) for Swift J1818.0−1607, for the short-duration (long-duration) search. Assuming isotropic emission of electromagnetic radiation of the burst fluences, we constrain the ratio of gravitational-wave energy to electromagnetic energy for bursts from SGR 1935+2154 with the available fluence information. The lowest of these ratios is 4.5 × 103
A joint Fermi-GBM and Swift-BAT analysis of gravitational-wave candidates from the third gravitational-wave observing run
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- Zhu Z.-H.
- Zimmerman A.B.
- Zucker M.E.
- Zweizig J.
- Publication venue
- American Astronomical Society
- Publication date
- 01/04/2024
- Field of study
Get PDFWe present Fermi Gamma-ray Burst Monitor (Fermi-GBM) and Swift Burst Alert Telescope (Swift-BAT) searches for gamma-ray/X-ray counterparts to gravitational-wave (GW) candidate events identified during the third observing run of the Advanced LIGO and Advanced Virgo detectors. Using Fermi-GBM onboard triggers and subthreshold gamma-ray burst (GRB) candidates found in the Fermi-GBM ground analyses, the Targeted Search and the Untargeted Search, we investigate whether there are any coincident GRBs associated with the GWs. We also search the Swift-BAT rate data around the GW times to determine whether a GRB counterpart is present. No counterparts are found. Using both the Fermi-GBM Targeted Search and the Swift-BAT search, we calculate flux upper limits and present joint upper limits on the gamma-ray luminosity of each GW. Given these limits, we constrain theoretical models for the emission of gamma rays from binary black hole mergers
Constraints on the cosmic expansion history from GWTC–3
- Author
- Abbott R.
- Abe H.
- Acernese F.
- Ackley K.
- Adhikari N.
- Adhikari R.X.
- Adkins V.K.
- Adya V.B.
- Affeldt C.
- Agarwal D.
- Agathos M.
- Agatsuma K.
- Aggarwal N.
- Aguiar O.D.
- Aiello L.
- Ain A.
- Ajith P.
- Akutsu T.
- Albanesi S.
- Alfaidi R.A.
- Allocca A.
- Altin P.A.
- Amato A.
- Anand C.
- Anand S.
- Ananyeva A.
- Anderson S.B.
- Anderson W.G.
- Ando M.
- Andrade T.
- Andres N.
- Andrić T.
- Andrés-Carcasona M.
- Angelova S.V.
- Ansoldi S.
- Antelis J.M.
- Antier S.
- Apostolatos T.
- Appavuravther E.Z.
- Appert S.
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- Arai K.
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- Arnaud N.
- Arogeti M.
- Aronson S.M.
- Arun K.G.
- Arène M.
- Asada H.
- Asali Y.
- Ashton G.
- Aso Y.
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- 'American Astronomical Society'
- Publication date
- 07/06/2023
- Field of study
Get PDFWe use 47 gravitational wave sources from the Third LIGO–Virgo–Kamioka Gravitational Wave Detector Gravitational Wave Transient Catalog (GWTC–3) to estimate the Hubble parameter H(z), including its current value, the Hubble constant H0. Each gravitational wave (GW) signal provides the luminosity distance to the source, and we estimate the corresponding redshift using two methods: the redshifted masses and a galaxy catalog. Using the binary black hole (BBH) redshifted masses, we simultaneously infer the source mass distribution and H(z). The source mass distribution displays a peak around 34 M⊙, followed by a drop-off. Assuming this mass scale does not evolve with the redshift results in a H(z) measurement, yielding H0=68−8+12km s−1Mpc−1 (68% credible interval) when combined with the H0 measurement from GW170817 and its electromagnetic counterpart. This represents an improvement of 17% with respect to the H0 estimate from GWTC–1. The second method associates each GW event with its probable host galaxy in the catalog GLADE+, statistically marginalizing over the redshifts of each event's potential hosts. Assuming a fixed BBH population, we estimate a value of H0=68−6+8km s−1Mpc−1 with the galaxy catalog method, an improvement of 42% with respect to our GWTC–1 result and 20% with respect to recent H0 studies using GWTC–2 events. However, we show that this result is strongly impacted by assumptions about the BBH source mass distribution; the only event which is not strongly impacted by such assumptions (and is thus informative about H0) is the well-localized event GW190814
The C/EBP family of transcription factors in the liver and other organs
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- Agre P.
- Akira S.
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- An M.R.
- Barone M.V.
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- Birkenmeier E.H.
- Bosch F.
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- Carlson S.G.
- Chang C.J.
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- Chen P.-L.
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- Chinery R.
- Chowdhury S.
- Christy R.J.
- Christy R.J.
- Chumakov A.M.
- Clarkson R.W.E.
- Cooper C.
- Costa R.H.
- Dai P.
- Descombes P.
- Descombes P.
- Diehl A.M.
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- Drolet D.W.
- Eckner R.
- Falvey E.
- Fornace A.J.
- Freytag S.O.
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- Hendricks-Taylor L.R.
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- Herbst R.S.
- Howell B.W.
- Hsu W.
- Hsu W.
- Hu E.
- Hunger S.P.
- Inaba T.
- Isshiki H.
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- Kageyama R.
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- Landschulz W.H.
- Landschulz W.H.
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- Leclair K.P.
- Lee Y.-H.
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- Lee Y.H.
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- Legraverend C.
- Lin F.-T.
- Lin F.T.
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- Trautwein C.
- Trautwein C.
- Tsukada J.
- Ubeda M.
- Umek R.M.
- Vallejo M.
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- Vietor I.
- Vinson C.R.
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- Wang N.-D.
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- Zinszner H.
- Zinszner H.
- Publication venue
- Blackwell Publishing
- Publication date
- Field of study
No full textMembers of the CCAAT/enhancer-binding protein (C/EBP) family of transcription factors are pivotal regulators of liver functions such as nutrient metabolism and its control by hormones, acute-phase response and liver regeneration. Recent progress in clarification of regulatory mechanisms for the C/EBP family members gives insight into understanding the liver functions at the molecular level
Search for gravitational-lensing signatures in the full third observing run of the LIGO-Virgo network
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- 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
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- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Alfaidi R.A
- Allocca A
- Alléné C
- Altin P.A
- Amato A
- Anand S
- Ananyeva A
- Anderson S.B
- Anderson W.G
- Ando M
- Andrade T
- Andres N
- Andrić T
- Andrés-Carcasona M
- Ansoldi S
- Antelis J.M
- Antier S
- Apostolatos T
- Appavuravther E.Z
- Appert S
- Apple S.K
- Arai K
- Araya A
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- Arellano F.E. Peña
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- Aronson S.M
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- Asada H
- Ashton G
- Aso Y
- Assiduo M
- Aston S.M
- Astone P
- Aubin F
- Aultoneal K
- Babak S
- Badaracco F
- Badger C
- Bae S
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- Bagnasco S
- Bai Y
- Baier J.G
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- Bartlett J
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- Bartos I
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- Bassiri R
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- Bernuzzi S
- Beroiz M
- Berry C.P.L
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- Bertolini A
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- Bianchi A
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- Bilicki M
- Billingsley G
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- Blackburn J.K
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- Bondarescu R
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- Yu Haocun
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- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 09/05/2023
- Field of study
No full textInternational audienceGravitational lensing by massive objects along the line of sight to the source causes distortions of gravitational wave-signals; such distortions may reveal information about fundamental physics, cosmology and astrophysics. In this work, we have extended the search for lensing signatures to all binary black hole events from the third observing run of the LIGO--Virgo network. We search for repeated signals from strong lensing by 1) performing targeted searches for subthreshold signals, 2) calculating the degree of overlap amongst the intrinsic parameters and sky location of pairs of signals, 3) comparing the similarities of the spectrograms amongst pairs of signals, and 4) performing dual-signal Bayesian analysis that takes into account selection effects and astrophysical knowledge. We also search for distortions to the gravitational waveform caused by 1) frequency-independent phase shifts in strongly lensed images, and 2) frequency-dependent modulation of the amplitude and phase due to point masses. None of these searches yields significant evidence for lensing. Finally, we use the non-detection of gravitational-wave lensing to constrain the lensing rate based on the latest merger-rate estimates and the fraction of dark matter composed of compact objects
Search for gravitational-lensing signatures in the full third observing run of the LIGO-Virgo network
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- Yeh S.-W
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- Yokoyama J
- Yokozawa T
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- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
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- Zanolin M
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- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 09/05/2023
- Field of study
No full textInternational audienceGravitational lensing by massive objects along the line of sight to the source causes distortions of gravitational wave-signals; such distortions may reveal information about fundamental physics, cosmology and astrophysics. In this work, we have extended the search for lensing signatures to all binary black hole events from the third observing run of the LIGO--Virgo network. We search for repeated signals from strong lensing by 1) performing targeted searches for subthreshold signals, 2) calculating the degree of overlap amongst the intrinsic parameters and sky location of pairs of signals, 3) comparing the similarities of the spectrograms amongst pairs of signals, and 4) performing dual-signal Bayesian analysis that takes into account selection effects and astrophysical knowledge. We also search for distortions to the gravitational waveform caused by 1) frequency-independent phase shifts in strongly lensed images, and 2) frequency-dependent modulation of the amplitude and phase due to point masses. None of these searches yields significant evidence for lensing. Finally, we use the non-detection of gravitational-wave lensing to constrain the lensing rate based on the latest merger-rate estimates and the fraction of dark matter composed of compact objects
Search for gravitational-lensing signatures in the full third observing run of the LIGO-Virgo network
- Author
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- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 09/05/2023
- Field of study
No full textInternational audienceGravitational lensing by massive objects along the line of sight to the source causes distortions of gravitational wave-signals; such distortions may reveal information about fundamental physics, cosmology and astrophysics. In this work, we have extended the search for lensing signatures to all binary black hole events from the third observing run of the LIGO--Virgo network. We search for repeated signals from strong lensing by 1) performing targeted searches for subthreshold signals, 2) calculating the degree of overlap amongst the intrinsic parameters and sky location of pairs of signals, 3) comparing the similarities of the spectrograms amongst pairs of signals, and 4) performing dual-signal Bayesian analysis that takes into account selection effects and astrophysical knowledge. We also search for distortions to the gravitational waveform caused by 1) frequency-independent phase shifts in strongly lensed images, and 2) frequency-dependent modulation of the amplitude and phase due to point masses. None of these searches yields significant evidence for lensing. Finally, we use the non-detection of gravitational-wave lensing to constrain the lensing rate based on the latest merger-rate estimates and the fraction of dark matter composed of compact objects
Search for subsolar-mass black hole binaries in the second part of Advanced LIGO's and Advanced Virgo's third observing run
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- Yeh S.-W
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- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 05/10/2023
- Field of study
No full textInternational audienceWe describe a search for gravitational waves from compact binaries with at least one component with mass 0.2 M⊙--1.0M⊙ and mass ratio q≥0.1 in Advanced LIGO and Advanced Virgo data collected between 1 November 2019, 15:00 UTC and 27 March 2020, 17:00 UTC. No signals were detected. The most significant candidate has a false alarm rate of 0.2 yr−1. We estimate the sensitivity of our search over the entirety of Advanced LIGO's and Advanced Virgo's third observing run, and present the most stringent limits to date on the merger rate of binary black holes with at least one subsolar-mass component. We use the upper limits to constrain two fiducial scenarios that could produce subsolar-mass black holes: primordial black holes (PBH) and a model of dissipative dark matter. The PBH model uses recent prescriptions for the merger rate of PBH binaries that include a rate suppression factor to effectively account for PBH early binary disruptions. If the PBHs are monochromatically distributed, we can exclude a dark matter fraction in PBHs fPBH≳0.6 (at 90% confidence) in the probed subsolar-mass range. However, if we allow for broad PBH mass distributions we are unable to rule out fPBH=1. For the dissipative model, where the dark matter has chemistry that allows a small fraction to cool and collapse into black holes, we find an upper bound fDBH<10−5 on the fraction of atomic dark matter collapsed into black holes
