362 research outputs found
Search for supersymmetric particles in scenarios with a gravitino LSP and stau NLSP
- Author
- Abreu P
- Adam W
- Adye T
- Adzic P
- Albrecht Z
- Alderweireld T
- Alekseev GD
- Alemany R
- Allmendinger T
- Allport PP
- Almehed S
- Amaldi U
- Amapane N
- Amato S
- Anassontzis EG
- Andersson P
- Andreazza A
- Andringa S
- Antilogus P
- Apel WD
- Arnoud Y
- Asman B
- Augustin JE
- Augustinus A
- Baillon P
- Ballestrero A
- Bambade P
- Barao F
- Barbiellini G
- Barbier R
- Bardin DY
- Barker G
- Baroncelli A
- Battaglia M
- Baubillier M
- Becks KH
- Begalli M
- Behrmann A
- Beilliere P
- Belokopytov Y
- Belous K
- Benekos NC
- Benvenuti AC
- Berat C
- Berggren M
- Bertrand D
- Besancon M
- Bilenky MS
- Bizouard MA
- Bloch D
- Blom HM
- Bonesini M
- Boonekamp M
- Booth PSL
- Borisov G
- Bosio C
- Botner O
- Boudinov E
- Bouquet B
- Bourdarios C
- Bowcock TJV
- Boyko I
- Bozovic I
- Bozzo M
- Bracko M
- Branchini P
- Brenner RA
- Bruckman P
- Brunet JM
- Bugge L
- Buran T
- Buschbeck B
- Buschmann P
- Caballero IG
- Cabrera S
- Caccia M
- Calvi M
- Camporesi T
- Canale V
- Carena F
- Carroll L
- Caso C
- Cattai A
- Cavallo FR
- Chabaud V
- Chapkin M
- Charpentier P
- Checchia P
- Chelkov GA
- Chierici R
- Chliapnikov P
- Chochula P
- Chorowicz V
- Chudoba J
- Cieslik K
- Collaboration DELPHI
- Collins P
- Contri R
- Cortina E
- Cosme G
- Cossutti F
- Costa M
- Crawley HB
- Crennell D
- Crepe S
- Crosetti G
- Czellar S
- Da Silva W
- Davenport M
- De Angelis A
- De Boer W
- De Clercq C
- De Lotto B
- De Min A
- De Paula L
- Della Ricca G
- Delpierre P
- Demaria N
- Di Ciaccio L
- Dijkstra H
- Dolbeau J
- Doroba K
- Dracos M
- Drees J
- Dris M
- Duperrin A
- Durand JD
- Eigen G
- Ekelof T
- Ekspong G
- Ellert M
- Elsing M
- Engel JP
- Fanourakis G
- Fassouliotis D
- Fayot J
- Feindt M
- Ferrer A
- Ferrer-Ribas E
- Ferro F
- Fichet S
- Firestone A
- Flagmeyer U
- Foeth H
- Fokitis E
- Fontanelli F
- Franek B
- Frodesen AG
- Fruhwirth R
- Fulda-Quenzer F
- Fuster J
- Galloni A
- Gamba D
- Gamblin S
- Gandelman M
- Garcia C
- Garcia SMI
- Gaspar C
- Gaspar M
- Gasparini U
- Gavillet P
- Gazis EN
- Gele D
- Geralis T
- Ghodbane N
- Gil I
- Gimenez MVC
- Glege F
- Gokieli R
- Golob B
- Gomez-Ceballos G
- Goncalves P
- Gopal G
- Gorn L
- Gouz Y
- Gracco V
- Grahl J
- Graziani E
- Gris P
- Grosdidier G
- Grzelak K
- Guy J
- Haag C
- Hahn F
- Hahn S
- Haider S
- Hallgren A
- Hamacher K
- Hansen J
- Harris FJ
- Hauler F
- Hedberg V
- Heising S
- Hernandez JJ
- Herquet P
- Herr H
- Hessing TL
- Heuser JM
- Higon E
- Holmgren SO
- Holt PJ
- Hoorelbeke S
- Houlden M
- Hrubec J
- Huber M
- Huet K
- Hughes GJ
- Hultqvist K
- Jackson JN
- Jacobsson R
- Jalocha P
- Janik R
- Jarlskog C
- Jarlskog G
- Jarry P
- Jean-Marie B
- Jeans D
- Johansson EK
- Jonsson P
- Joram C
- Juillot P
- Jungermann L
- Kapusta F
- Karafasoulis K
- Katsanevas S
- Katsoufis EC
- Keranen R
- Kernel G
- Kersevan BP
- Khokhlov Y
- Khomenko BA
- Khovanski NN
- Kiiskinen A
- King B
- Kinvig A
- Kjaer NJ
- Klapp O
- Klein H
- Kluit P
- Kokkinias P
- Kostioukhine V
- Kourkoumelis C
- Kouznetsov O
- Krammer M
- Kriznic E
- Krumstein Z
- Kubinec P
- Kurowska J
- Kurvinen K
- Lamsa JW
- Lane DW
- Lapin V
- Laugier JP
- Lauhakangas R
- Leder G
- Ledroit F
- Lefebure V
- Leinonen L
- Leisos A
- Leitner R
- Lenzen G
- Lepeltier V
- Lesiak T
- Lethuillier M
- Libby J
- Liebig W
- Liko D
- Lipniacka A
- Lippi I
- Loerstad B
- Loken JG
- Lopes JH
- Lopez JM
- Lopez-Fernandez R
- Loukas D
- Lutz P
- Lyons L
- MacNaughton J
- Maestro JC
- Mahon JR
- Maio A
- Malek A
- Malmgren TGM
- Maltezos S
- Malychev V
- Mandl F
- Marco J
- Marco R
- Marechal B
- Margoni M
- Marin JC
- Mariotti C
- Markou A
- Martinez-Rivero C
- Masik J
- Mastroyiannopoulos N
- Matorras F
- Matteuzzi C
- Matthiae G
- Mazzucato F
- Mazzucato M
- McCubbin M
- McKay R
- McNulty R
- McPherson G
- Meroni C
- Meyer WT
- Miagkov A
- Migliore E
- Mirabito L
- Mitaroff WA
- Mjoernmark U
- Moa T
- Moch M
- Moeller R
- Moenig K
- Monge MR
- Moraes D
- Moreau X
- Morettini P
- Morton G
- Mueller U
- Muenich K
- Mulders M
- Mulet-Marquis C
- Muresan R
- Murray WJ
- Muryn B
- Myatt G
- Myklebust T
- Naraghi F
- Nassiakou M
- Navarria FL
- Nawrocki K
- Negri P
- Neufeld N
- Nicolaidou R
- Nielsen BS
- Niezurawski P
- Nikolenko M
- Nomokonov V
- Nygren A
- Obraztsov V
- Olshevski AG
- Onofre A
- Orava R
- Orazi G
- Osterberg K
- Ouraou A
- Oyanguren A
- Paganoni M
- Paiano S
- Pain R
- Paiva R
- Palacios J
- Palka H
- Papadopoulou TD
- Pape L
- Parkes C
- Parodi F
- Parzefall U
- Passeri A
- Passon O
- Pavel T
- Pegoraro M
- Peralta L
- Pernicka M
- Perrotta A
- Petridou C
- Petrolini A
- Phillips HT
- Pierre F
- Pimenta M
- Piotto E
- Podobnik T
- Pol ME
- Polok G
- Poropat P
- Pozdniakov V
- Privitera P
- Pukhaeva N
- Pullia A
- Radojicic D
- Ragazzi S
- Rahmani H
- Rames J
- Ratoff PN
- Read AL
- Rebecchi P
- Redaelli NG
- Regler M
- Rehn J
- Reid D
- Reinertsen P
- Reinhardt R
- Renton PB
- Resvanis LK
- Richard F
- Ridky J
- Rinaudo G
- Ripp-Baudot I
- Rohne O
- Romero A
- Ronchese P
- Rosenberg EI
- Rosinsky P
- Roudeau P
- Rovelli T
- Royon C
- Ruhlmann-Kleider V
- Ruiz A
- Saarikko H
- Sacquin Y
- Sadovsky A
- Sajot G
- Salt J
- Sampsonidis D
- Sannino M
- Santo ME
- Schwemling P
- Schwering B
- Schwickerath U
- Scuri F
- Seager P
- Sedykh Y
- Segar AM
- Seibert N
- Sekulin R
- Shellard RC
- Siebel M
- Simard L
- Simonetto F
- Sisakian AN
- Smadja G
- Smirnova O
- Smith GR
- Solovianov O
- Sopczak A
- Sosnowski R
- Spassov T
- Spiriti E
- Squarcia S
- Stanescu C
- Stanic S
- Stanitzki M
- Stevenson K
- Stocchi A
- Strauss J
- Strub R
- Stugu B
- Szczekowski M
- Szeptycka M
- Tabarelli T
- Taffard A
- Tegenfeldt F
- Terranova F
- Thomas J
- Timmermans J
- Tinti N
- Tkatchev LG
- Tobin M
- Todorova S
- Tomaradze A
- Tome B
- Tonazzo A
- Tortora L
- Tortosa P
- Transtromer G
- Treille D
- Tristram G
- Trochimczuk M
- Troncon C
- Turluer ML
- Tyapkin IA
- Tyapkin P
- Tzamarias S
- Ullaland O
- Uvarov V
- Valenti G
- Vallazza E
- Van Dam P
- Van den Boeck W
- Van Eldik J
- Van Lysebetten A
- van Remortel N
- Van Vulpen I
- Vegni G
- Ventura L
- Venus W
- Verbeure F
- Verdier P
- Verlato M
- Vertogradov LS
- Verzi V
- Vilanova D
- Vitale L
- Vlasov E
- Vodopyanov AS
- Voulgaris G
- Vrba V
- Wahlen H
- Walck C
- Washbrook AJ
- Weiser C
- Wicke D
- Wickens JH
- Wilkinson GR
- Winter M
- Witek M
- Wolf G
- Yi J
- Yushchenko O
- Zalewska A
- Zalewski P
- Zavrtanik D
- Zevgolatakos E
- Zimin NI
- Zintchenko A
- Zoller P
- Zucchelli GC
- Zumerle G
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2000
- Field of study
Sleptons, neutralinos and charginos were searched for in the context of
scenarios where the lightest supersymmetric particle is the gravitino. It was
assumed that the stau is the next-to-lightest supersymmetric particle. Data
collected with the DELPHI detector at a centre-of-mass energy near 189 GeV were
analysed combining the methods developed in previous searches at lower
energies. No evidence for the production of these supersymmetric particles was
found. Hence, limits were derived at 95% confidence level.Comment: 31 pages, 14 figure
Measurement of Trilinear Gauge Couplings in e+e− Collisions at 161 GeV and 172 GeV
- Author
- Abreu P
- Adam W
- Adye T
- Adzic P
- Alekseev GD
- Alemany R
- Allport PP
- Almehed S
- Amaldi U
- Amato S
- Andersson P
- Andreazza A
- Antilogus P
- Apel WD
- Arnoud Y
- Asman B
- Augustin JE
- Augustinus A
- Baillon P
- Bambade P
- Barao F
- Barbier R
- Bardin DY
- Barker G
- Baroncelli A
- Barring O
- Bates MJ
- Battaglia M
- Baubillier M
- Becks KH
- Begalli M
- Beilliere P
- Belokopytov Y
- Benvenuti AC
- Berat C
- Berggren M
- Bertini D
- Bertrand D
- Besancon M
- Bianchi F
- Bigi M
- Bilenky MS
- Billoir P
- Bizouard MA
- Bloch D
- Bonesini M
- Bonivento W
- Boonekamp M
- Booth PSL
- Borgland AW
- Borisov G
- Bosio C
- Botner O
- Boudinov E
- Bouquet B
- Bourdarios C
- Bowcock TJV
- Bozovic I
- Bozzo M
- Branchini P
- Brand KD
- Brenke T
- Brenner RA
- Brown R
- Bruckman P
- Brunet JM
- Bugge L
- Buran T
- Burgsmueller T
- Buschmann P
- Caballero IG
- Cabrera S
- Caccia M
- Calvi M
- Camporesi T
- Canale V
- Canepa M
- Carena F
- Carroll L
- Caso C
- Cattai A
- Cavallo FR
- Cerruti C
- Chabaud V
- Chapkin M
- Charpentier P
- Chaussard L
- Checchia P
- Chelkov GA
- Chen M
- Chierici R
- Chliapnikov P
- Chochula P
- Chorowicz V
- Chudoba J
- Collaboration D
- Collins P
- Colomer M
- Contri R
- Cortina E
- Cosme G
- Cossutti F
- Cowell JH
- Crawley HB
- Crennell D
- Crosetti G
- Czellar S
- Da Silva W
- Dalmagne B
- Damgaard G
- Dauncey PD
- Davenport M
- De Angelis A
- De Boer W
- De Brabandere S
- De Clercq C
- De la Vaissiere C
- De Lotto B
- De Min A
- De Paula L
- Deghorain A
- Della Ricca G
- Delpierre P
- Demaria N
- Di Ciaccio L
- Di Diodato A
- Dijkstra H
- Djannati A
- Dolbeau J
- Doroba K
- Dracos M
- Drees J
- Drees KA
- Dris M
- Duperrin A
- Durand JD
- Edsall D
- Ehret R
- Eigen G
- Ekelof T
- Ekspong G
- Ellert M
- Elsing M
- Engel JP
- Erzen B
- Falk E
- Fanourakis G
- Fassouliotis D
- Fayot J
- Feindt M
- Ferrari P
- Ferrer A
- Fichet S
- Firestone A
- Fischer PA
- Flagmeyer U
- Foeth H
- Fokitis E
- Fontanelli F
- Formenti F
- Franek B
- Frodesen AG
- Fruhwirth R
- Fulda-Quenzer F
- Fuster J
- Galloni A
- Gamba D
- Gandelman M
- Garcia C
- Garcia J
- Garcia SM
- Gaspar C
- Gaspar M
- Gasparini U
- Gavillet P
- Gazis EN
- Gele D
- Gerber JP
- Gerdyukov L
- Ghodbane N
- Gimenez MVC
- Glege F
- Gokieli R
- Golob B
- Goncalves P
- Gopal G
- Gorn L
- Gorski M
- Gouz Y
- Gracco V
- Grahl J
- Graziani E
- Green C
- Grefrath A
- Gris P
- Grosdidier G
- Grzelak K
- Gunther M
- Guy J
- Hahn F
- Hahn S
- Haider S
- Hajduk Z
- Hallgren A
- Hamacher K
- Harris FJ
- Hedberg V
- Heising S
- Henriques R
- Hernandez JJ
- Herquet P
- Herr H
- Hessing TL
- Heuser JM
- Higon E
- Holmgren SO
- Holt PJ
- Holthuizen D
- Hoorelbeke S
- Houlden M
- Hrubec J
- Huet K
- Hultqvist K
- Jackson JN
- Jacobsson R
- Jalocha P
- Janik R
- Jarlskog C
- Jarlskog G
- Jarry P
- Jean-Marie B
- Johansson EK
- Jonsson L
- Jonsson P
- Joram C
- Juillot P
- Kapusta F
- Karafasoulis K
- Katsanevas S
- Katsoufis EC
- Keranen R
- Khomenko BA
- Khovanski NN
- King B
- Kjaer NJ
- Klapp O
- Klein H
- Kluit P
- Knoblauch D
- Kokkinias P
- Koratzinos M
- Korcyl K
- Kostioukhine V
- Kourkoumelis C
- Kouznetsov O
- Krammer M
- Kreuter C
- Kronkvist I
- Krumstein Z
- Kubinec P
- Kucewicz W
- Kurvinen K
- Lacasta C
- Lamsa JW
- Lanceri L
- Lane DW
- Langefeld P
- Lapin V
- Laugier JP
- Lauhakangas R
- Leder G
- Ledroit F
- Lefebure V
- Legan CK
- Leisos A
- Leitner R
- Lemonne J
- Lenzen G
- Lepeltier V
- Lesiak T
- Lethuillier M
- Libby J
- Liko D
- Lipniacka A
- Lippi I
- Loerstad B
- Loken JG
- Lopes JH
- Lopez JM
- Loukas D
- Lutz P
- Lyons L
- MacNaughton J
- Maestro JC
- Mahon JR
- Maio A
- Malek A
- Malmgren TGM
- Malychev V
- Mandl F
- Marco J
- Marco R
- Marechal B
- Margoni M
- Marin JC
- Mariotti C
- Markou A
- Martinez-Rivero C
- Martinez-Vidal F
- Matorras F
- Matteuzzi C
- Matthiae G
- Mazzucato F
- Mazzucato M
- Mc Cubbin M
- Mc Kay R
- Mc Nulty R
- Mc Pherson G
- Medbo J
- Meroni C
- Meyer WT
- Michelotto M
- Migliore E
- Mirabito L
- Mitaroff WA
- Mjoernmark U
- Moa T
- Moeller R
- Moenig K
- Monge MR
- Moreau X
- Morettini P
- Muenich K
- Mulders M
- Mundim LM
- Murray WJ
- Muryn B
- Myatt G
- Myklebust T
- Naraghi F
- Navarria FL
- Navas S
- Nawrocki K
- Negri P
- Nemecek S
- Neufeld N
- Neumann W
- Neumeister N
- Nicolaidou R
- Nielsen BS
- Nieuwenhuizen M
- Nikolaenko V
- Nikolenko M
- Niss P
- Nomerotski A
- Normand A
- Nygren A
- Oberschulte-Beckmann W
- Obraztsov V
- Olshevski AG
- Onofre A
- Orava R
- Orazi G
- Osterberg K
- Ouraou A
- Paganini P
- Paganoni M
- Paiano S
- Pain R
- Paiva R
- Palka H
- Papadopoulou TD
- Papageorgiou K
- Pape L
- Parkes C
- Parodi F
- Parzefall U
- Passeri A
- Pegoraro M
- Pernegger H
- Pernicka M
- Perrotta A
- Petridou C
- Petrolini A
- Phillips HT
- Piana G
- Pierre F
- Pimenta M
- Piotto E
- Podobnik T
- Podobrin O
- Pol ME
- Polok G
- Poropat P
- Pozdniakov V
- Privitera P
- Pukhaeva N
- Pullia A
- Radojicic D
- Ragazzi S
- Rahmani H
- Rames J
- Ratoff PN
- Read AL
- Rebecchi P
- Redaelli NG
- Regler M
- Reid D
- Reinhardt R
- Renton PB
- Resvanis LK
- Richard F
- Ridky J
- Rinaudo G
- Rohne O
- Romero A
- Ronchese P
- Rosenberg EI
- Rosinsky P
- Roudeau P
- Rovelli T
- Rozas AJC
- Ruhlmann-Kleiner V
- Ruiz A
- Saarikko H
- Sacquin Y
- Sadovsky A
- Sajot G
- Salt J
- Sampsonidis D
- Sannino M
- Santo ME
- Schneider H
- Schwickerath U
- Schyns MAE
- Scuri F
- Seager P
- Sedykh Y
- Segar AM
- Sekulin R
- Senko V
- Shellard RC
- Sheridan A
- Silvestre R
- Simonetto F
- Sisakian AN
- Skaali TB
- Smadja G
- Smirnov N
- Smirnova O
- Smith GR
- Solovianov O
- Sopczak A
- Sosnowski R
- Souza-Santos D
- Spassov T
- Spiriti E
- Sponholz P
- Squarcia S
- Stampfer D
- Stanescu C
- Stanic S
- Stapnes S
- Stavitski I
- Stevenson K
- Stocchi A
- Strauss J
- Strub R
- Stugu B
- Szczekowski M
- Szeptycka M
- Tabarelli T
- Tchikilev O
- Tegenfeldt F
- Terranova F
- Thomas J
- Tilquin A
- Timmermans J
- Tkatchev LG
- Todorov T
- Todorova S
- Toet DZ
- Tomaradze A
- Tome B
- Tonazzo A
- Tortora L
- Transtromer G
- Treille D
- Tristram G
- Trombini A
- Troncon C
- Tsirou A
- Turluer ML
- Tyapkin IA
- Tyndel M
- Tzamarias S
- Ueberschaer B
- Ullaland O
- Uvarov V
- Valenti G
- Vallazza E
- Van Apeldoorn GW
- Van Dam P
- Van Doninck WK
- Van Eldik J
- Van Lysebetten A
- Van Vulpen I
- Vassilopoulos N
- Vegni G
- Ventura L
- Venus W
- Verbeure F
- Verlato M
- Vertogradov LS
- Verzi V
- Vilanova D
- Vincent P
- Vishnevsky N
- Vitale L
- Vlasov E
- Vodopyanov AS
- Vrba V
- Wahlen H
- Walck C
- Waldner F
- Weiser C
- Wetherell AM
- Wicke D
- Wickens JH
- Wilkinson GR
- Williams WSC
- Winter M
- Witek M
- Wlodek T
- Wolf G
- Yi J
- Yushchenko O
- Zalewska A
- Zalewski P
- Zavrtanik D
- Zevgolatakos E
- Zimin NI
- Zucchelli GC
- Zumerle G
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/1997
- Field of study
Trilinear gauge boson couplings are measured using data taken by DELPHI at 161~GeV and 172~GeV. Values for WWV couplings (V=Z,γ) are determined from a study of the reactions \eeWW\ and \eeWev, using differential distributions from the WW final state in which one W decays hadronically and the other leptonically, and total cross-section data from other channels. Limits are also derived on neutral ZVγ couplings from an analysis of the reaction \eegi
Study of B0_s anti-B0_s oscillations and B0_s lifetimes using hadronic decays of B0_s mesons
- Author
- Abreu P
- Adam W
- Adye T
- Adzic P
- Ajinenko I
- Albrecht Z
- Alderweireld T
- Alekseev GD
- Alemany R
- Allmendinger T
- Allport PP
- Almehed S
- Amaldi U
- Amapane N
- Amato S
- Anassontzis EG
- Andersson P
- Andreazza A
- Andringa S
- Antilogus P
- Apel WD
- Arnoud Y
- Asman B
- Augustin JE
- Augustinus A
- Baillon P
- Bambade P
- Barao F
- Barbiellini G
- Barbier R
- Bardin DY
- Barker G
- Baroncelli A
- Battaglia M
- Baubillier M
- Becks KH
- Begalli M
- Behrman A
- Beilliere P
- Belokopytov Y
- Benekos NC
- Benvenuti AC
- Berat C
- Berggren M
- Bertini D
- Bertrand D
- Besancon M
- Bigi M
- Bilenky MS
- Bizouard MA
- Bloch D
- Blom HM
- Bonesini M
- Bonivento W
- Boonekamp M
- Booth PSL
- Borgland AW
- Borisov G
- Bosio C
- Botner O
- Boudinov E
- Bouquet B
- Bourdarios C
- Bowcock TJV
- Boyko I
- Bozovic I
- Bozzo M
- Bracko M
- Branchini P
- Brenke T
- Brenner RA
- Bruckman P
- Brunet JM
- Bugge L
- Buran T
- Burgsmueller T
- Buschbeck B
- Buschmann P
- Caballero IG
- Cabrera S
- Caccia M
- Calvi M
- Camporesi T
- Canale V
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2000
- Field of study
Oscillations of B0s mesons have been studied in samples selected from about
3.5 million hadronic Z decays detected by DELPHI between 1992 and 1995. One
analysis uses events in the exclusive decay channels: B0s -> Ds- pi+ or Ds- a1+
and B0s -> anti-D0 K- pi+ or anti-D0 K- a1+, where the D decays are completely
reconstructed. In addition, B0s anti-B0s oscillations have been studied in
events with an exclusively reconstructed Ds accompanied in the same hemisphere
by a high momentum hadron of opposite charge. Combining the two analyses, a
limit on the mass difference between the physical B0s states has been obtained:
Delta(m_B0s) > 4.0 ps^{-1} at the 95% C.L. with a sensitivity of Delta(m_B0s)
= 3.2 ps^{-1}. Using the latter sample of events, the B0s lifetime has been
measured and an upper limit on the decay width difference between the two
physical B0s states has been obtained:
tau(B0s) = 1.53^{+0.16}_{-0.15}(stat.) +/- {0.07}(syst.) ps
\Delta\Gamma(B0s)/\Gamma(B0s) < 0.69 at the 95% C.L.
The combination of these results with those obtained using Ds+- lepton-+
sample gives:
Delta(m_B0s) > 4.9 ps^{-1} at the 95% C.L.
with a sensitivity of Delta(m_B0s) = 8.7 ps^{-1}.
tau(B0s) = 1.46 +/- 0.11 ps and \Delta\Gamma(B0s)/\Gamma(B0s) < 0.45 at the
95% C.L.Comment: 42 pages, 13 figure
Multi-messenger observations of a binary neutron star merger
- Author
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- Manulis I
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- Middendorf L
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- Migoni Carlo
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- Mikhailov EE
- Milano L
- Milia Sabrina
- Miller AA
- Miller CJ
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- Moment G
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- Monzani ME
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- Moore CJ
- Moore RW
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- Morita K
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- Morris D
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- Morselli A
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- Moskalenko IV
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- Mostaf M
- Motohara K
- Moulai M
- Moulin E
- Mours B
- Moussa A
- Mow-Lowry CM
- Mrka S
- Mrka Z
- Mueller AL
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- Mueller BB
- Mueller G
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- Mueller MA
- Mueller S
- Muir AW
- Muir J
- Mukherjee Arunava
- Mukherjee D
- Mukherjee S
- Mukund N
- Mullavey A
- Munar-Adrover P
- Munch J
- Mundell CG
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- Murach T
- Murata KL
- Muratore M
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- Murphy T
- Murray PG
- Mussa R
- Myers ST
- Nagai H
- Nagashima H
- Nagayama T
- Nahnhauer R
- Nakahira S
- Nakajima M
- Nakamura Y
- Nakaoka T
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- Ohta K
- Oikonomou F
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- Ostrowski M
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- Ou G
- Overmier H
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- Pacciani L
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- Padilla N
- Padovani M
- Pagani C
- Page J
- Page KL
- Page MA
- Pai A
- Pai SA
- Pal-Singh A
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- Palashov O
- Palatiello M
- Palatka M
- Palazzi E
- Palczewski T
- Paliya VS
- Palliyaguru N
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- Pallot D
- Pallotta J
- Palmas S
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- Pant BC
- Panter M
- Paoletti F
- Paoletti F
- Paoli A
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- Papenbreer P
- Paragi Z
- Parente G
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- Perri LM
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- Perrodin D
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- Petrera S
- Petrucci P-O
- Peyaud B
- Pfeiffer HP
- Phelps M
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- Pian E
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- Pilia M
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- Pinard L
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- Piran T
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- Piranomonte S
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- Podsiadlowski P
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- Poggiani R
- Poh J
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- Pollmann A Obertacke
- Poolakkil S
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- Popa V
- Popolizio P
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- Porowski C
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- Powell J
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- Puppo P
- Qi H
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- Qu JL
- Quataert E
- Quel EJ
- Querchfeld S
- Querel R
- Quetschke V
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- Quinn L
- Quinn S
- Quinones C
- Quintero EA
- Quirrenbach A
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- Quitzow-James R
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- Raab FJ
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- Rabeling DS
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- Racca C
- Racusin J
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- Rain S
- Raja S
- Raja W
- Rajan C
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- Ramirez KE
- Ramirez-Ruiz E
- Ramos-Buades A
- Ramos-Pollan R
- Rana J
- Rando R
- Rao AR
- Rapagnani P
- Rappoldi A
- RATIR RIMAS
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- Raymond V
- Razza A
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- Razzaque S
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- Rea IC
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- Regimbau T
- Rei L
- Reichart DE
- Reid S
- Reimann R
- Reimer A
- Reimer A
- Reimer O
- Reimer O
- Reitze DH
- Relethford B
- Relich M
- Ren W
- Ren Z
- Renaud M
- Renzi V
- Reposeur T
- Resconi E
- Resmi L
- Rest A
- Reva IV
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- Reynolds T
- Rho CD
- Rhode W
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- Ricci F
- Ricci R
- Ricciarini S
- Riccobene G
- Richman M
- Ricker PM
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- Ridky J
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- Risse M
- Ristori P
- Rivera A Ramirez
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- Rizzo M
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- Robie R
- Robinet F
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- Rowan S
- Rowell G
- Rowlinson A
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- Roy R
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- Saito S
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- Sakamaki A
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- Sakellariadou M
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- Salazar H
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- Serino M
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- Serra-Ricart M
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- Steinlechner J
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- Tanimoto A
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- Tarle G
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- Tasson JD
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- Terreran G
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- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
GWTC-2.1: Deep extended catalog of compact binary coalescences observed by LIGO and Virgo during the first half of the third observing run
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- Wysocki DM
- Xiao L
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- Yang FW
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- Yang Z
- Yap MJ
- Yeeles DW
- Yelikar AB
- Ying M
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- Zadrożny A
- Zanolin M
- Zelenova T
- Zendri J-P
- Zevin M
- Zhang J
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- Zhang T
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- Zhao Yue
- Zhou R
- Zhou Z
- Zhu XJ
- Zimmerman AB
- Zlochower Y
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 15/01/2024
- Field of study
The second Gravitational-Wave Transient Catalog, GWTC-2, reported on 39 compact binary coalescences observed by the Advanced LIGO and Advanced Virgo detectors between 1 April 2019 15 ∶ 00 UTC and 1 October 2019 15 ∶ 00 UTC. Here, we present GWTC-2.1, which reports on a deeper list of candidate events observed over the same period. We analyze the final version of the strain data over this period with improved calibration and better subtraction of excess noise, which has been publicly released. We employ three matched-filter search pipelines for candidate identification, and estimate the probability of astrophysical origin for each candidate event. While GWTC-2 used a false alarm rate threshold of 2 per year, we include in GWTC-2.1, 1201 candidates that pass a false alarm rate threshold of 2 per day. We calculate the source properties of a subset of 44 high-significance candidates that have a probability of astrophysical origin greater than 0.5. Of these candidates, 36 have been reported in GWTC-2. We also calculate updated source properties for all binary black hole events previously reported in GWTC-1. If the eight additional high-significance candidates presented here are astrophysical, the mass range of events that are unambiguously identified as binary black holes (both objects ≥ 3 M⊙ ) is increased compared to GWTC-2, with total masses from ∼ 14 M ⊙ for GW190924_021846 to ∼ 182 M⊙ for GW190426_190642. Source properties calculated using our default prior suggest that the primary components of two new candidate events (GW190403_051519 and GW190426_190642) fall in the mass gap predicted by pair-instability supernova theory. We also expand the population of binaries with significantly asymmetric mass ratios reported in GWTC-2 by an additional two events (the mass ratio is less than 0.65 and 0.44 at 90% probability for GW190403_051519 and GW190917_114630 respectively), and find that two of the eight new events have effective inspiral spins χeff > 0 (at 90% credibility), while no binary is consistent with χeff < 0 at the same significance. We provide updated estimates for rates of binary black hole and binary neutron star coalescence in the local Universe
All-sky search for gravitational-wave bursts in the second joint LIGO-Virgo run
- Author
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- Atkinson D
- Aufmuth P
- Aulbert C
- Aylott BE
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- Khazanov EA
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- Kowalska I
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We present results from a search for gravitational-wave bursts in the data
collected by the LIGO and Virgo detectors between July 7, 2009 and October 20,
2010: data are analyzed when at least two of the three LIGO-Virgo detectors are
in coincident operation, with a total observation time of 207 days. The
analysis searches for transients of duration < 1 s over the frequency band
64-5000 Hz, without other assumptions on the signal waveform, polarization,
direction or occurrence time. All identified events are consistent with the
expected accidental background. We set frequentist upper limits on the rate of
gravitational-wave bursts by combining this search with the previous LIGO-Virgo
search on the data collected between November 2005 and October 2007. The upper
limit on the rate of strong gravitational-wave bursts at the Earth is 1.3
events per year at 90% confidence. We also present upper limits on source rate
density per year and Mpc^3 for sample populations of standard-candle sources.
As in the previous joint run, typical sensitivities of the search in terms of
the root-sum-squared strain amplitude for these waveforms lie in the range 5
10^-22 Hz^-1/2 to 1 10^-20 Hz^-1/2. The combination of the two joint runs
entails the most sensitive all-sky search for generic gravitational-wave bursts
and synthesizes the results achieved by the initial generation of
interferometric detectors.Comment: 15 pages, 7 figures: data for plots and archived public version at
https://dcc.ligo.org/cgi-bin/DocDB/ShowDocument?docid=70814&version=19, see
also the public announcement at
http://www.ligo.org/science/Publication-S6BurstAllSky
All-sky search for continuous gravitational waves from isolated neutron stars in the early O3 LIGO data
- Author
- Abbott R
- Abbott TD
- Abraham S
- Acernese F
- Ackley K
- Adams A
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- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Aleman KM
- Allen G
- Allocca A
- Altin PA
- Amato A
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
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- Angelova S
- Ansoldi S
- Antelis JM
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- Areeda JS
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- Xiao L
- Xu W-R
- Yamada T
- Yamamoto H
- Yamamoto Kazuhiro
- Yamamoto Kohei
- Yamamoto T
- Yamashita K
- Yamazaki R
- Yang FW
- Yang L
- Yang Yang
- Yang Yi
- Yang Z
- Yap MJ
- Yeeles DW
- Yelikar AB
- Ying M
- Yokogawa K
- Yokoyama J
- Yokozawa T
- Yoon A
- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
- Zanolin M
- Zeidler S
- Zelenova T
- Zendri J-P
- Zevin M
- Zhan M
- Zhang H
- Zhang J
- Zhang L
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- Zhang T
- Zhao C
- Zhao G
- Zhao Yue
- Zhao Yuhang
- Zhou Z
- Zhu XJ
- Zhu Z-H
- Zucker ME
- Zweizig J
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 15/10/2021
- Field of study
We report on an all-sky search for continuous gravitational waves in the frequency band 20-2000 Hz and with a frequency time derivative in the range of [-1.0,+0.1]×10-8 Hz/s. Such a signal could be produced by a nearby, spinning and slightly nonaxisymmetric isolated neutron star in our Galaxy. This search uses the LIGO data from the first six months of Advanced LIGO's and Advanced Virgo's third observational run, O3. No periodic gravitational wave signals are observed, and 95% confidence-level (C.L.) frequentist upper limits are placed on their strengths. The lowest upper limits on worst-case (linearly polarized) strain amplitude h0 are ∼1.7×10-25 near 200 Hz. For a circularly polarized source (most favorable orientation), the lowest upper limits are ∼6.3×10-26. These strict frequentist upper limits refer to all sky locations and the entire range of frequency derivative values. For a population-averaged ensemble of sky locations and stellar orientations, the lowest 95% C.L. upper limits on the strain amplitude are ∼1.4×10-25. These upper limits improve upon our previously published all-sky results, with the greatest improvement (factor of ∼2) seen at higher frequencies, in part because quantum squeezing has dramatically improved the detector noise level relative to the second observational run, O2. These limits are the most constraining to date over most of the parameter space searched
All-sky, all-frequency directional search for persistent gravitational waves from Advanced LIGO’s and Advanced Virgo’s first three observing runs
- Author
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- Wysocki DM
- Xiao L
- Xu W-R
- Yamada T
- Yamamoto H
- Yamamoto Kazuhiro
- Yamamoto Kohei
- Yamamoto T
- Yamashita K
- Yamazaki R
- Yang FW
- Yang L
- Yang Y
- Yang Yang
- Yang Z
- Yap MJ
- Yeeles DW
- Yelikar AB
- Ying M
- Yokogawa K
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeidler S
- Zelenova T
- Zendri J-P
- Zevin M
- Zhan M
- Zhang H
- Zhang J
- Zhang L
- Zhang T
- Zhang Y
- Zhao C
- Zhao G
- Zhao Y
- Zhao Yue
- Zhou R
- Zhou Z
- Zhu XJ
- Zhu Z-H
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 03/06/2022
- Field of study
We present the first results from an all-sky all-frequency (ASAF) search for
an anisotropic stochastic gravitational-wave background using the data from the
first three observing runs of the Advanced LIGO and Advanced Virgo detectors.
Upper limit maps on broadband anisotropies of a persistent stochastic
background were published for all observing runs of the LIGO-Virgo detectors.
However, a broadband analysis is likely to miss narrowband signals as the
signal-to-noise ratio of a narrowband signal can be significantly reduced when
combined with detector output from other frequencies. Data folding and the
computationally efficient analysis pipeline, {\tt PyStoch}, enable us to
perform the radiometer map-making at every frequency bin. We perform the search
at 3072 {\tt{HEALPix}} equal area pixels uniformly tiling the sky and in every
frequency bin of width 1/32~Hz in the range 20−1726~Hz, except for bins
that are likely to contain instrumental artefacts and hence are notched. We do
not find any statistically significant evidence for the existence of narrowband
gravitational-wave signals in the analyzed frequency bins. Therefore, we place
95% confidence upper limits on the gravitational-wave strain for each
pixel-frequency pair, the limits are in the range (0.030−9.6)×10−24. In addition, we outline a method to identify candidate
pixel-frequency pairs that could be followed up by a more sensitive (and
potentially computationally expensive) search, e.g., a matched-filtering-based
analysis, to look for fainter nearly monochromatic coherent signals. The ASAF
analysis is inherently independent of models describing any spectral or spatial
distribution of power. We demonstrate that the ASAF results can be
appropriately combined over frequencies and sky directions to successfully
recover the broadband directional and isotropic results
Effects of coal rank on physicochemical properties of coal and on methane adsorption
- Author
- A Busch
- A Busch
- A Busch
- A Ciembroniewicz
- A Hildenbrand
- A Marecka
- A Nodzeński
- A Saghafi
- AE DeGance
- AP Radliński
- AV Astashov
- B Dutka
- B Taraba
- BD Banerjee
- BG Kutchko
- C Laxminarayana
- C Laxminarayana
- C Özgen Karacan
- CR Clarkson
- CR Clarkson
- CR Clarkson
- D Charrière
- DF Zhang
- DJ Allardice
- E Battistutta
- E Yalçin
- FH An
- G Ceglarska-Stefańska
- GR Barker-Read
- GRL Chalmers
- H Gan
- H Jin
- H Martyniuk
- H Yu
- H Yu
- HG Yu
- HG Yu
- HJ Kim
- HL Lin
- HZ Chang
- HZ Chang
- J Bae
- J Milewska-Duda
- J Wang
- JD Giuliani
- JDN Pone
- JE Fitzgerald
- JF Unsworth
- JH Levy
- JI Joubert
- JI Joubert
- JJ Chaback
- JR Nelson
- JY Jiang
- KK Bhattacharyya
- L Xu
- M Faiz
- M Mastalerz
- M Mastalerz
- MC He
- MH Reich
- MM Faiz
- N Gal Le
- N Siemons
- OP Mahajan
- P Dutta
- PJ Crosdale
- PJ Crosdale
- PJ Reucroft
- Q Zhang
- QL Zhang
- QL Zhang
- QL Zhang
- R Pini
- R Pini
- R Sakurovs
- RM Bustin
- RT Yang
- S Chen
- S Dai
- S Day
- S Day
- S Hao
- S Kędzior
- S Mazumder
- SP Nandi
- SX Hao
- SY Zhang
- SY Zhang
- T Maphala
- TE Mares
- WI Friesen
- WJ Zhang
- WJ Zou
- XB Su
- XB Su
- XH Fu
- XH Fu
- XH Fu
- XZ Ma
- Y Cai
- Y Cai
- Y Gensterblum
- Y Yao
- Y Yao
- YB Li
- YJ Yu
- Z Majewska
- Z Majewska
- Z Majewska
- Z Pan
- Z Weishauptová
- ZG Xiao
- ZH Chen
- ZH Qin
- ZN Liu
- ZY Yang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for gravitational waves associated with gamma-ray bursts detected by Fermi and Swift during the LIGO–Virgo run O3b
- Author
- Abbott R
- Abbott TD
- Acernese F
- Ackley K
- Adams C
- Adhikari N
- Adhikari RX
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Allocca A
- Altin PA
- Amato A
- Anand C
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Andrade T
- Andres N
- Andric T
- Angelova SV
- Ansoldi S
- Antelis JM
- Antier S
- Appert S
- Arai K
- Arai K
- Arai Y
- Araki S
- Araya A
- Araya MC
- Areeda JS
- Arellano FEP
- Arene M
- Aritomi N
- Arnaud N
- Aronson SM
- Arun KG
- Asada H
- Asali Y
- Ashton G
- Aso Y
- Assiduo M
- Aston SM
- Astone P
- Aubin F
- Austin C
- Babak S
- Badaracco F
- Bader MKM
- Badger C
- Bae S
- Bae Y
- Baer AM
- Bagnasco S
- Bai Y
- Baiotti L
- Baird J
- Bajpai R
- Ball M
- Ballardin G
- Ballmer SW
- Balsamo A
- Baltus G
- Banagiri S
- Bankar D
- Barayoga JC
- Barbieri C
- Barish BC
- Barker D
- Barneo P
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Barton MA
- Bartos I
- Bassiri R
- Basti A
- Bawaj M
- Bayley JC
- Baylor AC
- Bazzan M
- Becsy B
- Bedakihale VM
- Bejger M
- Belahcene I
- Benedetto V
- Beniwal D
- Bennett TF
- Bentley JD
- BenYaala M
- Bergamin F
- Berger BK
- Bernuzzi S
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- Beveridge D
- Bhandare R
- Bhardwaj U
- Bhattacharjee D
- Bhaumik S
- Bilenko IA
- Billingsley G
- Bini S
- Birney R
- Birnholtz O
- Biscans S
- Bischi M
- Biscoveanu S
- Bisht A
- Biswas B
- Bitossi M
- Bizouard M-A
- Blackburn JK
- Blair CD
- Blair DG
- Blair RM
- Bobba F
- Bode N
- Boer M
- Bogaert G
- Boldrini M
- Bonavena LD
- Bondu F
- Bonilla E
- Bonnand R
- Booker P
- Boom BA
- Bork R
- Boschi V
- Bose N
- Bose S
- Bossilkov V
- Boudart V
- Bouffanais Y
- Bozzi A
- Bradaschia C
- Brady PR
- Bramley A
- Branch A
- Branchesi M
- Brau JE
- Breschi M
- Briant T
- Briggs JH
- Brillet A
- Brinkmann M
- Brockill P
- Brooks AF
- Brooks J
- Brown DD
- Brunett S
- Bruno G
- Bruntz R
- Bryant J
- Bulik T
- Bulten HJ
- Buonanno A
- Buscicchio R
- Buskulic D
- Bustillo JC
- Buy C
- Byer RL
- Cadonati L
- Cagnoli G
- Cahillane C
- Callaghan JD
- Callister TA
- Calloni E
- Cameron J
- Camp JB
- Canepa M
- Canevarolo S
- Cannavacciuolo M
- Cannon KC
- Canton TD
- Cao H
- Cao Z
- Capocasa E
- Capote E
- Carapella G
- Carbognani F
- Carlin JB
- Carney MF
- Carpinelli M
- Carrillo G
- Carullo G
- Carver TL
- Casentini C
- Castaldi G
- Caudill S
- Cavaglia M
- Cavalier F
- Cavalieri R
- Ceasar M
- Cella G
- Cerda-Duran P
- Cesarini E
- Chaibi W
- Chakravarti K
- Champion E
- Chan C
- Chan C-H
- Chan CL
- Chan K
- Chan M
- Chandra K
- Chanial P
- Chao S
- Charlton P
- Chase EA
- Chassande-Mottin E
- Chatterjee C
- Chatterjee D
- Chatterjee D
- Chaturvedi M
- Chaty S
- Chatziioannou K
- Chen C
- Chen HY
- Chen J
- Chen K
- Chen X
- Chen Y-B
- Chen Y-R
- Chen Z
- Cheng H
- Cheong CK
- Cheung HY
- Chia HY
- Chiadini F
- Chiang C-Y
- Chiarini G
- Chierici R
- Chincarini A
- Chiofalo ML
- Chiummo A
- Cho G
- Cho HS
- Choudhary RK
- Choudhary S
- Christensen N
- Chu H
- Chu Q
- Chu Y-K
- Chua S
- Chung KW
- Ciani G
- Ciecielag P
- Cieslar M
- Cifaldi M
- Ciobanu AA
- Ciolfi R
- Cipriano F
- Cirone A
- Clara F
- Clark EN
- Clark JA
- Clarke L
- Clearwater P
- Clesse S
- Cleva F
- Coccia E
- Codazzo E
- Cohadon P-F
- Cohen DE
- Cohen L
- Collaboration KAGRA
- Collaboration LIGOS
- Collaboration LIGOS
- Collaboration V
- Collaboration V
- Colleoni M
- Collette CG
- Colombo A
- Colpi M
- Compton CM
- Conti L
- Cooper SJ
- Corban P
- Corbitt TR
- Cordero-Carrion I
- Corezzi S
- Corley KR
- Cornish N
- Corre D
- Corsi A
- Cortese S
- Costa CA
- Cotesta R
- Coughlin MW
- Coulon J-P
- Countryman ST
- Cousins B
- Couvares P
- Coward DM
- Cowart MJ
- Coyne DC
- Coyne R
- Creighton JDE
- Creighton TD
- Criswell AW
- Croquette M
- Crowder SG
- Cudell JR
- Cullen TJ
- Cumming A
- Cummings R
- Cunningham L
- Cuoco E
- Curylo M
- D'Angelo B
- D'Antonio S
- D'Emilio V
- D'Onofrio L
- D'Urso D
- Dabadie P
- Dall'Osso S
- Dalya G
- Dana A
- DaneshgaranBajastani LM
- Danilishin S
- Danzmann K
- Darsow-Fromm C
- Dasgupta A
- Datrier LEH
- Datta S
- Dattilo V
- Dave I
- Davier M
- Davies GS
- Davis D
- Davis MC
- Daw EJ
- De Lillo F
- De Lillo N
- De Matteis F
- De Pietri R
- De Rosa R
- De Rossi C
- De Simone R
- Dean R
- DeBra D
- Deenadayalan M
- Degallaix J
- Del Favero V
- Del Pozzo W
- Deleglise S
- DeMarchi LM
- 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 Pace S
- Di Palma I
- Di Renzo F
- Diaz JC
- Diaz MC
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- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2022
- Field of study
We search for gravitational-wave signals associated with gamma-ray bursts (GRBs) detected by the Fermi and Swift satellites during the second half of the third observing run of Advanced LIGO and Advanced Virgo (2019 November 1 15:00 UTC–2020 March 27 17:00 UTC). We conduct two independent searches: a generic gravitational-wave transients search to analyze 86 GRBs and an analysis to target binary mergers with at least one neutron star as short GRB progenitors for 17 events. We find no significant evidence for gravitational-wave signals associated with any of these GRBs. A weighted binomial test of the combined results finds no evidence for subthreshold gravitational-wave signals associated with this GRB ensemble either. We use several source types and signal morphologies during the searches, resulting in lower bounds on the estimated distance to each GRB. Finally, we constrain the population of low-luminosity short GRBs using results from the first to the third observing runs of Advanced LIGO and Advanced Virgo. The resulting population is in accordance with the local binary neutron star merger rate
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