340 research outputs found
Development of Advanced Photon Calibrator for KAGRA
- Author
- Publication venue
- Publication date
- 23/02/2023
- Field of study
The KAGRA cryogenic gravitational-wave observatory has begun joint
observation with the worldwide gravitational waves detector network. Precise
calibration of the detector response is essential for the parameter estimation
of gravitational wave sources. The photon calibrator is the main calibrator in
LIGO, Virgo and KAGRA, and we used this calibrator in joint observation 3 on
2020 April with GEO600 in Germany. KAGRA improved the system for joint
observation 3 with three unique points: high laser power, power stabilization
system, and remote beam position control. KAGRA employs the 20 W laser and
divides it into two beams injected on the mirror surface. By using a high-power
laser, we can calibrate the response at the kHz region. To control the power of
each laser independently, we also installed an optical follower servo for each
beam power stabilization. By controlling the optical path of the photon
calibrater beam positions with pico-motors, we were able to characterize the
rotation response of the detector. We also installed a telephoto camera and QPD
to monitor beam position and controlled beam position to optimize mirror
response. In this paper, we discussed the statistical error with the result of
the relative power noise measurement. We also discussed systematic errors about
the power calibration model of photon calibrator and simulation of elastic
deformation effect with the finite element analysis.Comment: 16 pages, 10 figure
KAGRA: 2.5 Generation Interferometric Gravitational Wave Detector
- Author
- Akutsu T.
- Ando M.
- Arai K.
- Arai Y.
- Araki S.
- Araya A.
- Arellano F. E. P.
- Aritomi N.
- Asada H.
- Aso Y.
- Atsuta S.
- Awai K.
- Bae S.
- Baiotti L.
- Barton M. A.
- Cannon K.
- Capocasa E.
- Chen C. -S.
- Chiu T. -W.
- Cho K.
- Chu Y. -K.
- Craig K.
- Creus W.
- Doi K.
- Eda K.
- Enomoto Y.
- Flaminio R.
- Fujii Y.
- Fujimoto M. -K.
- Fukunaga M.
- Fukushima M.
- Furuhata T.
- Haino S.
- Hasegawa K.
- Hashino K.
- Hayama K.
- Hirobayashi S.
- Hirose E.
- Hsieh B. H.
- Huang C. -Z.
- Ikenoue B.
- Inoue Y.
- Ioka K.
- Itoh Y.
- Izumi K.
- Kaji T.
- Kajita T.
- Kakizaki M.
- Kamiizumi M.
- Kanbara S.
- Kanda N.
- Kanemura S.
- Kaneyama M.
- Kang G.
- Kasuya J.
- Kataoka Y.
- Kawai N.
- Kawamura S.
- Kawasaki T.
- Kim C.
- Kim J.
- Kim J. C.
- Kim W. S.
- Kim Y. -M.
- Kimura N.
- Kinugawa T.
- Kirii S.
- Kitaoka Y.
- Kitazawa H.
- Kojima Y.
- Kokeyama K.
- Komori K.
- Kong A. K. H.
- Kotake K.
- Kozu R.
- Kumar R.
- Kuo H. -S.
- Kuroyanagi S.
- Lee H. K.
- Lee H. M.
- Lee H. W.
- Leonardi M.
- Lin C. -Y.
- Lin F. -L.
- Liu G. C.
- Liu Y.
- Majorana E.
- Mano S.
- Marchio M.
- Martin E. N. T. S.
- Matsui T.
- Matsushima F.
- Michimura Y.
- Mio N.
- Miyakawa O.
- Miyamoto A.
- Miyamoto T.
- Miyo K.
- Miyoki S.
- Morii W.
- Morisaki S.
- Moriwaki Y.
- Morozumi T.
- Musha M.
- Nagano K.
- Nagano S.
- Nakamura K.
- Nakamura T.
- Nakano H.
- Nakano M.
- Nakao K.
- Narikawa T.
- Naticchioni L.
- Ni W. -T.
- Nishizawa A.
- Obuchi Y.
- Ochi T.
- Oh J. J.
- Oh S. H.
- Ohashi M.
- Ohishi N.
- Ohkawa M.
- Okutomi K.
- Ono K.
- Oohara K.
- Ooi C. P.
- Pan S. -S.
- Park J.
- Pinto I.
- Quynh L. N.
- Sago N.
- Saijo M.
- Saito Y.
- Saitou S.
- Sakai K.
- Sakai Y.
- Sakai Y.
- Sasai M.
- Sasaki M.
- Sasaki Y.
- Sato N.
- Sato S.
- Sato T.
- Sekiguchi Y.
- Seto N.
- Shibata M.
- Shimoda T.
- Shinkai H.
- Shishido T.
- Shoda A.
- Somiya K.
- Son E. J.
- Suemasa A.
- Suzuki T.
- Suzuki T.
- Tagoshi H.
- Tahara H.
- Takahashi H.
- Takahashi R.
- Takamori A.
- Takeda H.
- Tanaka H.
- Tanaka K.
- Tanaka T.
- Tanioka S.
- Tatsumi D.
- Tomaru T.
- Tomura T.
- Travasso F.
- Tsubono K.
- Tsuchida S.
- Uchikata N.
- Uchiyama T.
- Uehara T.
- Ueki S.
- Ueno K.
- Uraguchi F.
- Ushiba T.
- van Putten M. H. P. M.
- Vocca H.
- Wada S.
- Wakamatsu T.
- Watanabe Y.
- Xu W. -R.
- Yamada T.
- Yamamoto A.
- Yamamoto K.
- Yamamoto K.
- Yamamoto S.
- Yamamoto T.
- Yokogawa K.
- Yokoyama J.
- Yokozawa T.
- Yoon T. H.
- Yoshioka T.
- Yuzurihara H.
- Zeidler S.
- Zhu Z. -H.
- Publication venue
- Publication date
- 20/11/2018
- Field of study
The recent detections of gravitational waves (GWs) reported by LIGO/Virgocollaborations have made significant impact on physics and astronomy. A globalnetwork of GW detectors will play a key role to solve the unknown nature of thesources in coordinated observations with astronomical telescopes and detectors.Here we introduce KAGRA (former name LCGT; Large-scale Cryogenic Gravitationalwave Telescope), a new GW detector with two 3-km baseline arms arranged in theshape of an "L", located inside the Mt. Ikenoyama, Kamioka, Gifu, Japan.KAGRA's design is similar to those of the second generations such as AdvancedLIGO/Virgo, but it will be operating at the cryogenic temperature with sapphiremirrors. This low temperature feature is advantageous for improving thesensitivity around 100 Hz and is considered as an important feature for thethird generation GW detector concept (e.g. Einstein Telescope of Europe orCosmic Explorer of USA). Hence, KAGRA is often called as a 2.5 generation GWdetector based on laser interferometry. The installation and commissioning ofKAGRA is underway and its cryogenic systems have been successfully tested inMay, 2018. KAGRA's first observation run is scheduled in late 2019, aiming tojoin the third observation run (O3) of the advanced LIGO/Virgo network. In thiswork, we describe a brief history of KAGRA and highlights of main feature. Wealso discuss the prospects of GW observation with KAGRA in the era of O3. Whenoperating along with the existing GW detectors, KAGRA will be helpful to locatea GW source more accurately and to determine the source parameters with higherprecision, providing information for follow-up observations of a GW triggercandidate
Vibration isolation system with a compact damping system for power recycling mirrors of KAGRA
- Author
- Akiyama Y.
- Akutsu T.
- Ando M.
- Arai K.
- Arai Y.
- Araki S.
- Araya A.
- Aritomi N.
- Asada H.
- Aso Y.
- Bae S.
- Baiotti L.
- Barton M. A.
- Cannon K.
- Capocasa E.
- Chen C. -S.
- Chiu T. -W.
- Cho K.
- Chu Y. -K.
- Craig K.
- Dattilo V.
- Doi K.
- Enomoto Y.
- Flaminio R.
- Fujii Y.
- Fujimoto M. -K.
- Fukunaga M.
- Fukushima M.
- Furuhata T.
- Haino S.
- Hasegawa K.
- Hashimoto Y.
- Hashino K.
- Hayama K.
- Hirayama T.
- Hirose E.
- Hsieh B. H.
- Huang C. -Z.
- Ikenoue B.
- Inoue Y.
- Ioka K.
- Itoh Y.
- Izumi K.
- Kaji T.
- Kajita T.
- Kakizaki M.
- Kamiizumi M.
- Kanbara S.
- Kanda N.
- Kanemura S.
- Kang G.
- Kasuya J.
- Kawai N.
- Kawasaki T.
- Kim C.
- Kim J.
- Kim J. C.
- Kim W. S.
- Kimura N.
- Kirii S.
- Kitaoka Y.
- Kitazawa H.
- Kojima Y.
- Kokeyama K.
- Komori K.
- Kong A.
- Kotake K.
- Kozu R.
- Kumar R.
- Kuo H. -S.
- Kuroki S.
- Kuroyanagi S.
- Lee H. K.
- Lee H. M.
- Lee H. W.
- Leonardi M.
- Lin C. -Y.
- Lin F. -L.
- Liu G. C.
- Marchio M.
- Matsui T.
- Michimura Y.
- Mio N.
- Miyakawa O.
- Miyamoto A.
- Miyoki S.
- Morii W.
- Morisaki S.
- Moriwaki Y.
- Musha M.
- Nagano K.
- Nagano S.
- Nakamura K.
- Nakamura T.
- Nakano H.
- Nakano M.
- Narikawa T.
- Nguyen Quynh L.
- Ni W. -T.
- Nishizawa A.
- Obuchi Y.
- Oh J.
- Oh S. H.
- Ohashi M.
- Ohishi N.
- Ohkawa M.
- Okutomi K.
- Ono K.
- Oohara K.
- Ooi C. P.
- Pan S. -S.
- Paoletti F.
- Park J.
- Passaquieti R.
- Pena Arellano F. E.
- Sago N.
- Saito S.
- Saito Y.
- Sakai K.
- Sakai Y.
- Sasai M.
- Sato S.
- Sato T.
- Sekiguchi T.
- Sekiguchi Y.
- Shibata M.
- Shimoda T.
- Shinkai H.
- Shishido T.
- Shoda A.
- Someya N.
- Somiya K.
- Son E. J.
- Suemasa A.
- Suzuki T.
- Suzuki T.
- Tagoshi H.
- Tahara H.
- Takahashi H.
- Takahashi R.
- Takeda H.
- Tanaka H.
- Tanaka K.
- Tanaka T.
- Tanioka S.
- Tapia San Martin E. N.
- Tomaru T.
- Tomura T.
- Travasso F.
- Tsubono K.
- Tsuchida S.
- Uchikata N.
- Uchiyama T.
- Uehara T.
- Ueno K.
- Uraguchi F.
- Ushiba T.
- Van Putten M. H. P. M.
- Vocca H.
- Wakamatsu T.
- Watanabe Y.
- Xu W. -R.
- Yamada T.
- Yamamoto K.
- Yamamoto K.
- Yamamoto S.
- Yamamoto T.
- Yokogawa K.
- Yokoyama J.
- Yokozawa T.
- Yoshioka T.
- Yuzurihara H.
- Zeidler S.
- Zhu Z. -H.
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
A vibration isolation system called the Type-Bp system used for power recycling mirrors has been developed for KAGRA, the interferometric gravitational-wave observatory in Japan. A suspension of the Type-Bp system passively isolates an optic from seismic vibration using three main pendulum stages equipped with two vertical vibration isolation systems. A compact reaction mass around each of the main stages allows for achieving sufficient damping performance with a simple feedback as well as vibration isolation ratio. Three Type-Bp systems were installed in KAGRA, and were proved to satisfy the requirements on the damping performance, and also on estimated residual displacement of the optics
Aerobic nonylphenol degradation and nitro-nonylphenol formation by microbial cultures from sediments
- Author
- A Navarro
- A Soares
- Alette Langenhoff
- AS Snyder
- B Thiele
- BV Chang
- C Shannon
- CR Tyler
- E Stephanou
- F-X Yang
- FLP Gabriel
- FLP Gabriel
- GA LeBlanc
- H Zhang
- H-P Koops
- H-PE Kohler
- Huub Rijnaarts
- J Krooneman
- J Weert de
- Jasperien De Weert
- LY Stein
- M Hesselsoe
- M Petrovic
- Marc Viñas
- ME Tros
- MJH Telscher
- MR Hyman
- MR Servos
- OP Heemken
- PFX Corvini
- PFX Corvini
- PFX Corvini
- R Ekelund
- S Lacorte
- S-G Hou
- S-H Baek
- SY Yuan
- T Tanghe
- TF Wheeler
- Tim Grotenhuis
- U Kammann
- W Giger
- WG Weisburg
- WK Keener
- Y Ushiba
- Y Xiao
- YP Vries de
- Z Yu
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2010
- Field of study
Nonylphenol (NP) is an estrogenic pollutant which is widely present in the aquatic environment. Biodegradation of NP can reduce the toxicological risk. In this study, aerobic biodegradation of NP in river sediment was investigated. The sediment used for the microcosm experiments was aged polluted with NP. The biodegradation of NP in the sediment occurred within 8 days with a lag phase of 2 days at 30°C. During the biodegradation, nitro-nonylphenol metabolites were formed, which were further degraded to unknown compounds. The attached nitro-group originated from the ammonium in the medium. Five subsequent transfers were performed from original sediment and yielded a final stable population. In this NP-degrading culture, the microorganisms possibly involved in the biotransformation of NP to nitro-nonylphenol were related to ammonium-oxidizing bacteria. Besides the degradation of NP via nitro-nonylphenol, bacteria related to phenol-degrading species, which degrade phenol via ring cleavage, are abundantly present
Search for continuous gravitational waves from 20 accreting millisecond x-ray pulsars in O3 LIGO data
- Author
- Abbott R
- Abbott T
- Acernese F
- Ackley K
- Adams C
- Adhikari N
- Adhikari R
- Adya V
- Affeldt C
- Agarwal D
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar O
- Aiello L
- Ain A
- Akutsu T
- Albanesi S
- Albayati A
- Allocca A
- Altamirano D
- Altin P
- Amato A
- Anand C
- Anand S
- Ananyeva A
- Anderson S
- Anderson W
- Ando M
- Andrade T
- Andres N
- Andrić T
- Angelova S
- Ansoldi S
- Antelis J
- Antier S
- Appert S
- Arai K
- Arai Y
- Araki S
- Araya A
- Araya M
- Areeda J
- Arellano FP
- Aritomi N
- Arnaud N
- Aronson S
- Arun K
- Arène M
- Asada H
- Asali Y
- Ashton G
- Aso Y
- Assiduo M
- Aston S
- Astone P
- Aubin F
- Austin C
- Babak S
- Badaracco F
- Bader M
- Badger C
- Bae S
- Bae Y
- Baer A
- Bagnasco S
- Bai Y
- Baiotti L
- Baird J
- Bajpai R
- Ball M
- Ballardin G
- Ballmer S
- Balsamo A
- Baltus G
- Banagiri S
- Bankar D
- Barayoga J
- Barbieri C
- Barish B
- Barker D
- Barneo P
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Barton M
- Bartos I
- Bassiri R
- Basti A
- Bawaj M
- Bayley J
- Baylor A
- Bazzan M
- Bedakihale V
- Bejger M
- Belahcene I
- Benedetto V
- Beniwal D
- Bennett T
- Bentley J
- BenYaala M
- Bergamin F
- Berger B
- Bernuzzi S
- Bersanetti D
- Bertolini A
- Betzwieser J
- Beveridge D
- Bhandare R
- Bhardwaj U
- Bhattacharjee D
- Bhaumik S
- Bilenko I
- Billingsley G
- Bini S
- Birney R
- Birnholtz O
- Biscans S
- Bischi M
- Biscoveanu S
- Bisht A
- Biswas B
- Bitossi M
- Bizouard M
- Blackburn J
- Blair C
- Blair D
- Blair R
- Bobba F
- Bode N
- Boer M
- Bogaert G
- Boldrini M
- Bonavena L
- Bondu F
- Bonilla E
- Bonnand R
- Booker P
- Boom B
- Bork R
- Boschi V
- Bose N
- Bose S
- Bossilkov V
- Boudart V
- Bouffanais Y
- Bozzi A
- Bradaschia C
- Brady P
- Bramley A
- Branch A
- Branchesi M
- Brau J
- Breschi M
- Briant T
- Briggs J
- Brillet A
- Brinkmann M
- Brockill P
- Brooks A
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- Bruno G
- Bruntz R
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- Bulik T
- Bult P
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- Buonanno A
- Buscicchio R
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- Buy C
- Byer R
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- Cagnoli G
- Cahillane C
- Callaghan J
- Callister T
- Calloni E
- Cameron J
- Camp J
- Canepa M
- Canevarolo S
- Cannavacciuolo M
- Cannon K
- Canton TD
- Cao H
- Cao Z
- Capocasa E
- Capote E
- Carapella G
- Carbognani F
- Carlin J
- Carney M
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- Carrillo G
- Carullo G
- Carver T
- Casentini C
- Castaldi G
- Caudill S
- Cavaglià M
- Cavalier F
- Cavalieri R
- Ceasar M
- Cella G
- Cerdá-Durán P
- Cesarini E
- Chaibi W
- Chakrabarty D
- Chakravarti K
- Champion E
- Chan C
- Chan K
- Chan M
- Chandra K
- Chanial P
- Chao S
- Charlton P
- Chase E
- Chassande-Mottin E
- Chatterjee C
- Chatterjee D
- Chaturvedi M
- Chaty S
- Chen C
- Chen H
- Chen J
- Chen K
- Chen X
- Chen Y
- Chen Z
- Cheng H
- Cheong C
- Cheung H
- Chia H
- Chiadini F
- Chiang C
- Chiarini G
- Chierici R
- Chincarini A
- Chiofalo M
- Chiummo A
- Cho G
- Cho H
- Choudhary R
- Choudhary S
- Christensen N
- Chu H
- Chu Q
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- Chung K
- Ciani G
- Ciecielag P
- Cieślar M
- Cifaldi M
- Ciobanu A
- Ciolfi R
- Cipriano F
- Cirone A
- Clara F
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- Clearwater P
- Clesse S
- Cleva F
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- Codazzo E
- Cohadon P
- Cohen D
- Cohen L
- Colleoni M
- Collette C
- Colombo A
- Colpi M
- Compton C
- Constancio M
- Conti L
- Cooper S
- Corban P
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- Cordero-Carrión I
- Corezzi S
- Corley K
- Cornish N
- Corre D
- Corsi A
- Cortese S
- Costa C
- Cotesta R
- Coughlin M
- Coulon J
- Countryman S
- Cousins B
- Couvares P
- Coward D
- Cowart M
- Coyne D
- Coyne R
- Creighton J
- Creighton T
- Criswell A
- Croquette M
- Crowder S
- Cudell J
- Cullen T
- Cumming A
- Cummings R
- Cunningham L
- Cuoco E
- Curyło M
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- Dana A
- DaneshgaranBajastani L
- Danilishin S
- Danzmann K
- Darsow-Fromm C
- Dasgupta A
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- Datta S
- Dattilo V
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- Degallaix J
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- Deléglise S
- DeMarchi L
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- Depasse A
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- Dhurandhar S
- Di Fiore L
- Di Fronzo C
- Di Giorgio C
- Di Giovanni F
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- Di Girolamo T
- Di Lieto A
- Di Pace S
- Di Palma I
- Di Renzo F
- Diaz JC
- Diaz-Ortiz M
- Didio N
- Dietrich T
- Ding B
- Divakarla A
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- Doctor Z
- Donovan F
- Dooley K
- Doravari S
- Dorrington I
- Drago M
- Driggers J
- Drori Y
- Ducoin J
- Dupej P
- Durante O
- Duverne P
- Dwyer S
- Dálya G
- Díaz M
- D’Angelo B
- D’Antonio S
- D’Emilio V
- D’Onofrio L
- D’Urso D
- e Melo IT
- Eassa C
- Easter P
- Ebersold M
- Eckhardt T
- Eddolls G
- Edelman B
- Edo T
- Edy O
- Effler A
- Eguchi S
- Eichholz J
- Eikenberry S
- Eisenmann M
- Eisenstein R
- Ejlli A
- Engelby E
- Enomoto Y
- Errico L
- Essick R
- Estellés H
- Estevez D
- Etienne Z
- Etzel T
- Evans M
- Evans T
- Ewing B
- Fafone V
- Fair H
- Fairhurst S
- Farah A
- Farinon S
- Farr B
- Farr W
- Farrow N
- Fauchon-Jones E
- Favaro G
- Favata M
- Fays M
- Fazio M
- Feicht J
- Fejer M
- Fenyvesi E
- Ferguson D
- Fernandez-Galiana A
- Ferrante I
- Ferreira T
- Fidecaro F
- Figura P
- Fiori I
- Fishbach M
- Fisher R
- Fittipaldi R
- Fiumara V
- Flaminio R
- Floden E
- Fong H
- Font J
- Fornal B
- Forsyth P
- Franke A
- Frasca S
- Frasconi F
- Frederick C
- Freed J
- Frei Z
- Freise A
- Frey R
- Fritschel P
- Frolov V
- Fronzé G
- Fujii Y
- Fujikawa Y
- Fukunaga M
- Fukushima M
- Fulda P
- Fyffe M
- Gabbard H
- Gadre B
- Gair J
- Gais J
- Galaudage S
- Gamba R
- Ganapathy D
- Ganguly A
- Gao D
- Gaonkar S
- Garaventa B
- García-Núñez C
- García-Quirós C
- Garufi F
- Gateley B
- Gaudio S
- Gayathri V
- Ge G
- Gemme G
- Gennai A
- George J
- Gerberding O
- Gergely L
- Gewecke P
- Ghonge S
- Ghosh A
- Ghosh S
- Giacomazzo B
- Giacoppo L
- Giaime J
- Giardina K
- Gibson D
- Gier C
- Giesler M
- Giri P
- Gissi F
- Glanzer J
- Gleckl A
- Godwin P
- Goetz E
- Goetz R
- Gohlke N
- Goncharov B
- González G
- Gopakumar A
- Gosselin M
- Gouaty R
- Gould D
- Grace B
- Grado A
- Granata M
- Granata V
- Grant A
- Gras S
- Grassia P
- Gray C
- Gray R
- Greco G
- Green A
- Green R
- Gretarsson A
- Gretarsson E
- Griffith D
- Griffiths W
- Griggs H
- Grignani G
- Grimaldi A
- Grimm S
- Grote H
- Grunewald S
- Gruning P
- Guerra D
- Guidi G
- Guimaraes A
- Guixé G
- Gulati H
- Guo H
- Guo Y
- Gupta A
- Gupta P
- Gustafson E
- Gustafson R
- Guzman F
- Ha S
- Haegel L
- Hagiwara A
- Haino S
- Halim O
- Hall E
- Hamilton E
- Hammond G
- Han W
- Haney M
- Hanks J
- Hanna C
- Hannam M
- Hannuksela O
- Hansen H
- Hansen T
- Hanson J
- Harder T
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
Search for gravitational waves from Scorpius X-1 with a hidden Markov model in O3 LIGO data
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhikari N
- Adhikari R
- Adkins V
- Adya V
- Affeldt C
- Agarwal D
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar O
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Alfaidi R
- Allocca A
- Altin P
- Amato A
- Anand C
- Anand S
- Ananyeva A
- Anderson S
- Anderson W
- Ando M
- Andrade T
- Andres N
- Andrić T
- Andrés-Carcasona M
- Angelova S
- Ansoldi S
- Antelis J
- Antier S
- Apostolatos T
- Appavuravther E
- Appert S
- Apple S
- Arai K
- Araya A
- Araya M
- Areeda J
- Arellano F
- Aritomi N
- Arnaud N
- Arogeti M
- Aronson S
- Arène M
- Asada H
- Asali Y
- Ashton G
- Aso Y
- Assiduo M
- Aston S
- Astone P
- Aubin F
- AultONeal K
- Austin C
- Babak S
- Badaracco F
- Bader M
- Badger C
- Bae S
- Bae Y
- Baer A
- Bagnasco S
- Bai Y
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- Bajpai R
- Baka T
- Ball M
- Ballardin G
- Ballmer S
- Balsamo A
- Baltus G
- Banagiri S
- Banerjee B
- Bankar D
- Barayoga J
- Barbieri C
- Barish B
- Barker D
- Barneo P
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Barton M
- Bartos I
- Basak S
- Bassiri R
- Basti A
- Bawaj M
- Bayley J
- Bazzan M
- Becher B
- Bedakihale V
- Beirnaert F
- Bejger M
- Belahcene I
- Benedetto V
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- BenYaala M
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- Cesarini E
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- van Haevermaet H
- van Heijningen J
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- van Remortel N
- Vander-Hyde D
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- Wysocki D
- Xiao L
- Yamada T
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- Yamashita K
- Yamazaki R
- Yang F
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- Yap M
- Yeeles D
- Yeh S
- Yelikar A
- Ying M
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu H
- Yuzurihara H
- Zadrożny A
- Zanolin M
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- Zevin M
- Zhan M
- Zhang H
- Zhang J
- Zhang L
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- Zimmerman A
- Zucker M
- Zweizig J
- Publication venue
- Publication date
- 01/01/2022
- Field of study
All-sky search for short gravitational-wave bursts in the third Advanced LIGO and Advanced Virgo run
- Author
- Abbott R
- Abbott T
- Acernese F
- Ackley K
- Adams C
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
Constraints on the cosmic expansion history from GWTC-3
- Author
- Abbott R.
- Abe H.
- Acernese F.
- Ackley K.
- Adhikari N.
- Adhikari R.
- Adkins V.
- Adya V.
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- Publication venue
- Publication date
- 19/11/2021
- Field of study
We use 47 gravitational-wave sources from the Third LIGO-Virgo-KAGRA 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 34M⊙, followed by a drop-off. Assuming this mass scale does not evolve with redshift results in a H(z) measurement, yielding H0=68−7+12kms−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+8kms−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
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