47 research outputs found
Localization and broadband follow-up of the gravitational-wave transient GW150914
- Author
- Abbott BP
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- Abdalla FB
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- Publication venue
- Astrophysical Journal Letters
- Publication date
- 01/01/2016
- Field of study
A gravitational-wave (GW) transient was identified in data recorded by the Advanced Laser Interferometer Gravitational-wave Observatory (LIGO) detectors on 2015 September 14. The event, initially designated G184098 and later given the name GW150914, is described in detail elsewhere. By prior arrangement, preliminary estimates of the time, significance, and sky location of the event were shared with 63 teams of observers covering radio, optical, near-infrared, X-ray, and gamma-ray wavelengths with ground- and space-based facilities. In this Letter we describe the low-latency analysis of the GW data and present the sky localization of the first observed compact binary merger. We summarize the follow-up observations reported by 25 teams via private Gamma-ray Coordinates Network circulars, giving an overview of the participating facilities, the GW sky localization coverage, the timeline, and depth of the observations. As this event turned out to be a binary black hole merger, there is little expectation of a detectable electromagnetic (EM) signature. Nevertheless, this first broadband campaign to search for a counterpart of an Advanced LIGO source represents a milestone and highlights the broad capabilities of the transient astronomy community and the observing strategies that have been developed to pursue neutron star binary merger events. Detailed investigations of the EM data and results of the EM follow-up campaign are being disseminated in papers by the individual teams
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: GW170817 and GRB 170817A
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- Zertuche LM
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- Zhu SJ
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- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17, the gravitational-wave event GW170817 was observed by the Advanced LIGO and Virgo detectors, and the gamma-ray burst (GRB) GRB 170817A was observed independently by the Fermi Gamma-ray Burst Monitor, and the Anti-Coincidence Shield for the Spectrometer for the International Gamma-Ray Astrophysics Laboratory. The probability of the near-simultaneous temporal and spatial observation of GRB 170817A and GW170817 occurring by chance is 5.0×10−8. We therefore confirm binary neutron star mergers as a progenitor of short GRBs. The association of GW170817 and GRB 170817A provides new insight into fundamental physics and the origin of short GRBs. We use the observed time delay of (+1.74±0.05)s between GRB 170817A and GW170817 to: (i) constrain the difference between the speed of gravity and the speed of light to be between −3×10−15 and +7×10−16 times the speed of light, (ii) place new bounds on the violation of Lorentz invariance, (iii) present a new test of the equivalence principle by constraining the Shapiro delay between gravitational and electromagnetic radiation. We also use the time delay to constrain the size and bulk Lorentz factor of the region emitting the gamma-rays. GRB 170817A is the closest short GRB with a known distance, but is between 2 and 6 orders of magnitude less energetic than other bursts with measured redshift. A new generation of gamma-ray detectors, and subthreshold searches in existing detectors, will be essential to detect similar short bursts at greater distances. Finally, we predict a joint detection rate for the Fermi Gamma-ray Burst Monitor and the Advanced LIGO and Virgo detectors of 0.1-1.4 per year during the 2018-2019 observing run and 0.3-1.7 per year at design sensitivity
Multi-messenger observations of a binary neutron star merger
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- Aartsen MG
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- Piro AL
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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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- 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, all-frequency directional search for persistent gravitational waves from Advanced LIGO’s and Advanced Virgo’s first three observing runs
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- 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
All-sky search for continuous gravitational waves from isolated neutron stars in the early O3 LIGO data
- Author
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- Abbott TD
- Abraham S
- Acernese F
- Ackley K
- Adams A
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- Adya VB
- Affeldt C
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- Aleman KM
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- Arnaud N
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- Trovato A
- Trozzo L
- Trudeau RJ
- Tsai D
- Tsai DS
- Tsang KW
- Tsang T
- Tsao J-S
- Tse M
- Tso R
- Tsubono K
- Tsuchida S
- Tsukada L
- Tsuna D
- Tsutsui T
- Tsuzuki T
- Turconi M
- Tuyenbayev D
- Ubhi AS
- Uchikata N
- Uchiyama T
- Udall RP
- Ueda A
- Uehara T
- Ueno K
- Ueshima G
- Ugolini D
- Unnikrishnan CS
- Uraguchi F
- Urban AL
- Ushiba T
- Usman SA
- Utina AC
- Vahlbruch H
- Vajente G
- Vajpeyi A
- Valdes G
- Valentini M
- Valsan V
- van Bakel N
- van Beuzekom M
- van den Brand JFJ
- Van den Broeck C
- van der Schaaf L
- van Heijningen J
- van Putten MHPM
- Vander-Hyde DC
- Vanosky J
- Vardaro M
- Vargas AF
- Varma V
- Vasuth M
- Vecchio A
- Vedovato G
- Veitch J
- Veitch PJ
- Venkateswara K
- Venneberg J
- Venugopalan G
- Verkindt D
- Verma Y
- Veske D
- Vetrano F
- Vicere A
- Viets AD
- Villa-Ortega V
- Vinet J-Y
- Vitale S
- Vivanco F Hernandez
- Vo T
- Vocca H
- von Reis ERG
- von Wrangel J
- Vorvick C
- Vyatchanin SP
- Wade LE
- Wade M
- Wagner KJ
- Walet RC
- Walker M
- Wallace GS
- Wallace L
- Walsh S
- Wang J
- Wang JZ
- Wang WH
- Ward RL
- Warner J
- Was M
- Washimi T
- Washington NY
- Watchi J
- Weaver B
- Wei L
- Weinert M
- Weinstein AJ
- Weiss R
- Weldon G
- Weller CM
- Wellmann F
- Wen L
- Wessels P
- Westhouse JW
- Wette K
- Whelan JT
- White DD
- Whiting BF
- Whittle C
- Wilken D
- Williams D
- Williams MJ
- Williamson AR
- Willis JL
- Willke B
- Wilson DJ
- Winkler W
- Wipf CC
- Wlodarczyk T
- Woan G
- Woehler J
- Wofford JK
- Wong ICF
- Wu C
- Wu DS
- Wu H
- Wu S
- 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 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
- Zhang R
- 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
Recommended from our members
Prospects for Observing and Localizing Gravitational-Wave Transients with Advanced LIGO and Advanced Virgo.
- Author
- Abbott BP
- Abbott R
- Abbott TD
- Abernathy MR
- Acernese F
- Ackley K
- Adams C
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Ain A
- Ajith P
- Allen B
- Allocca A
- Altin PA
- Amariutei DV
- Anderson SB
- Anderson WG
- Arai K
- Araya MC
- Arceneaux CC
- Areeda JS
- Arnaud N
- Arun KG
- Ashton G
- Ast M
- Aston SM
- Astone P
- Aufmuth P
- Aulbert C
- Babak S
- Baker PT
- Baldaccini F
- Ballardin G
- Ballmer SW
- Barayoga JC
- Barclay SE
- Barish BC
- Barker D
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Bartos I
- Bassiri R
- Basti A
- Batch JC
- Baune C
- Bavigadda V
- Bazzan M
- Behnke B
- Bejger M
- Belczynski C
- Bell AS
- Bell CJ
- Berger BK
- Bergman J
- Bergmann G
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- Bhagwat S
- Bhandare R
- Bilenko IA
- Billingsley G
- Birch J
- Birney R
- Biscans S
- Bisht A
- Bitossi M
- Biwer C
- Bizouard MA
- Blackburn JK
- Blair CD
- Blair D
- Blair RM
- Bloemen S
- Bock O
- Bodiya TP
- Boer M
- Bogaert G
- Bogan C
- Bohe A
- Bojtos P
- Bond C
- Bondu F
- Bonnand R
- Bork R
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- Bozzi A
- Bradaschia C
- Brady PR
- Braginsky VB
- Branchesi M
- Brau JE
- Briant T
- Brillet A
- Brinkmann M
- Brisson V
- Brockill P
- Brooks AF
- Brown DA
- Brown DD
- Brown NM
- Buchanan CC
- Buikema A
- Bulik T
- Bulten HJ
- Buonanno A
- Buskulic D
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- Byer RL
- Cadonati L
- Cagnoli G
- Cahillane C
- Calderón Bustillo J
- Callister T
- Calloni E
- Camp JB
- Cannon KC
- Cao J
- Capano CD
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- Carbognani F
- Caride S
- Casanueva Diaz J
- Casentini C
- Castro JM Gonzalez
- Caudill S
- Cavaglià M
- Cavalier F
- Cavalieri R
- Cella G
- Cepeda C
- Cerboni Baiardi L
- Cerretani G
- Cesarini E
- Chakraborty R
- Chalermsongsak T
- Chamberlin SJ
- Chan M
- Chao S
- Charlton P
- Chassande-Mottin E
- Chen HY
- Chen Y
- Cheng C
- Chincarini A
- Chiummo A
- Cho HS
- Cho M
- Chow JH
- Christensen N
- Chu Q
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- Cleva F
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- Collette CG
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- Coughlin SB
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- Countryman ST
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- Cowart MJ
- Coyne DC
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- Crowder SG
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- Drever RWP
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- Eikenberry SS
- Engels W
- Essick RC
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- Jiménez-Forteza F
- Johnson WW
- Jones DI
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- Kalogera V
- Kandhasamy S
- Kang G
- Kanner JB
- Karki S
- Kasprzack M
- Katsavounidis E
- Katzman W
- Kaufer S
- Kaur T
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- Kawazoe F
- Kehl MS
- Keitel D
- Kelley DB
- Kells W
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- Kinzel DL
- Kissel JS
- Kleybolte L
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- Koehlenbeck SM
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- Koley S
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- Kontos A
- Korobko M
- Korth WZ
- Kowalska I
- Kozak DB
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- Lee HM
- Lee K
- Lenon A
- Leonardi M
- Leong JR
- Leroy N
- Letendre N
- Levin Y
- Levine BM
- Li TGF
- Libson A
- LIGO Scientific Collaboration
- Littenberg TB
- Lockerbie NA
- Logue J
- Lombardi AL
- Lord JE
- Lorenzini M
- Loriette V
- Lormand M
- Losurdo G
- Lough JD
- Lundgren AP
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- Machenschalk B
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- Macleod DM
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- Magee RM
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- Martin IW
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- Massinger TJ
- Masso-Reid M
- Matichard F
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- McClelland DE
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- McWilliams ST
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- Merzougui M
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- Messenger C
- Messick C
- Meyers PM
- Mezzani F
- Miao H
- Michel C
- Middleton H
- Mikhailov EE
- Milano L
- Miller J
- Millhouse M
- Minenkov Y
- Ming J
- Mirshekari S
- Mishra C
- Mitra S
- Mitrofanov VP
- Mitselmakher G
- Mittleman R
- Moggi A
- Mohan M
- Mohapatra SRP
- Montani M
- Moore BC
- Moore CJ
- Moraru D
- Moreno G
- Morriss SR
- Mossavi K
- Mours B
- Mow-Lowry CM
- Mueller CL
- Mueller G
- Muir AW
- Mukherjee Arunava
- Mukherjee D
- Mukherjee S
- Mullavey A
- Munch J
- Murphy DJ
- Murray PG
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- Márka S
- Márka Z
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- Naticchioni L
- Nayak RK
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- Nedkova K
- Nelemans G
- Neri M
- Neunzert A
- Newton G
- Nguyen TT
- Nielsen AB
- Nissanke S
- Nitz A
- Nocera F
- Nolting D
- Normandin MEN
- Nuttall LK
- O'Dell J
- O'Reilly B
- O'Shaughnessy R
- Oberling J
- Ochsner E
- Oelker E
- Ogin GH
- Oh JJ
- Oh SH
- Ohme F
- Oliver M
- Oppermann P
- Oram RJ
- Ott CD
- Ottaway DJ
- Ottens RS
- Overmier H
- Owen BJ
- Pai A
- Pai SA
- Pal-Singh A
- Palamos JR
- Palashov O
- Palomba C
- Pan H
- Pankow C
- Pannarale F
- Pant BC
- Paoletti F
- Paoli A
- Papa MA
- Paris HR
- Parker W
- Pascucci D
- Pasqualetti A
- Passaquieti R
- Passuello D
- Patrick Z
- Pearlstone BL
- Pedraza M
- Pedurand R
- Pekowsky L
- Pele A
- Penn S
- Pereira R
- Perreca A
- Phelps M
- Piccinni O
- Pichot M
- Piergiovanni F
- Pierro V
- Pillant G
- Pinard L
- Pinto IM
- Pitkin M
- Poggiani R
- Post A
- Powell J
- Prasad J
- Predoi V
- Premachandra SS
- Prestegard T
- Price LR
- Prijatelj M
- Principe M
- Privitera S
- Prodi GA
- Prokhorov L
- Punturo M
- Puppo P
- Pürrer M
- Qi H
- Qin J
- Quetschke V
- Quintero EA
- Quitzow-James R
- Raab FJ
- Rabeling DS
- Radkins H
- Raffai P
- Raja S
- Rakhmanov M
- Rapagnani P
- Raymond V
- Razzano M
- Re V
- Read J
- Reed CM
- Regimbau T
- Rei L
- Reid S
- Reitze DH
- Rew H
- Ricci F
- Riles K
- Robertson NA
- Robie R
- Robinet F
- Rocchi A
- Rolland L
- Rollins JG
- Roma VJ
- Romano JD
- Romano R
- Romanov G
- Romie JH
- Rosińska D
- Rowan S
- Ruggi P
- Ryan K
- Rüdiger A
- Sachdev S
- Sadecki T
- Sadeghian L
- Saleem M
- Salemi F
- Samajdar A
- Sammut L
- Sanchez EJ
- Sandberg V
- Sandeen B
- Sanders JR
- Sassolas B
- Sathyaprakash BS
- Saulson PR
- Sauter O
- Savage RL
- Sawadsky A
- Schale P
- Schilling R
- Schmidt J
- Schmidt P
- Schnabel R
- Schofield RMS
- Schreiber E
- Schuette D
- Schutz BF
- Schönbeck A
- Scott J
- Scott SM
- Sellers D
- Sentenac D
- Sequino V
- Sergeev A
- Serna G
- Setyawati Y
- Sevigny A
- Shaddock DA
- Shah S
- Shahriar MS
- Shaltev M
- Shao Z
- Shapiro B
- Shawhan P
- Sheperd A
- Shoemaker DH
- Shoemaker DM
- Siellez K
- Siemens X
- Sigg D
- Silva AD
- Simakov D
- Singer A
- Singer LP
- Singh A
- Singh R
- Sintes AM
- Slagmolen BJJ
- Smith JR
- Smith ND
- Smith RJE
- Son EJ
- Sorazu B
- Sorrentino F
- Souradeep T
- Srivastava AK
- Staley A
- Steinke M
- Steinlechner J
- Steinlechner S
- Steinmeyer D
- Stephens BC
- Stone R
- Strain KA
- Straniero N
- Stratta G
- Strauss NA
- Strigin S
- Sturani R
- Stuver AL
- Summerscales TZ
- Sun L
- Sutton PJ
- Swinkels BL
- Szczepanczyk MJ
- Tacca M
- Talukder D
- Tanner DB
- Tarabrin SP
- Taracchini A
- Taylor R
- Theeg T
- Thirugnanasambandam MP
- Thomas EG
- Thomas M
- Thomas P
- Thorne KA
- Thorne KS
- Thrane E
- Tiwari S
- Tiwari V
- Tokmakov KV
- Tomlinson C
- Tonelli M
- Torres CV
- Torrie CI
- Travasso F
- Traylor G
- Trifirò D
- Tringali MC
- Trozzo L
- Tse M
- Turconi M
- Tuyenbayev D
- Tápai M
- Töyrä D
- Ugolini D
- Unnikrishnan CS
- Urban AL
- Usman SA
- Vahlbruch H
- Vajente G
- Valdes G
- van Bakel N
- van Beuzekom M
- van den Brand JFJ
- van den Broeck C
- van der Schaaf L
- van der Sluys MV
- van Heijningen JV
- van Veggel AA
- Vander-Hyde DC
- Vardaro M
- Vass S
- Vasúth M
- Vaulin R
- Vecchio A
- Vedovato G
- Veitch J
- Veitch PJ
- Venkateswara K
- Verkindt D
- Vetrano F
- Viceré A
- Vinciguerra S
- Vine DJ
- Vinet J-Y
- Virgo Collaboration
- Vitale S
- Vo T
- Vocca H
- Vorvick C
- Vousden WD
- Vyatchanin SP
- Wade AR
- Wade LE
- Wade M
- Walker M
- Wallace L
- Walsh S
- Wang G
- Wang H
- Wang M
- Wang X
- Wang Y
- Ward RL
- Warner J
- Was M
- Weaver B
- Wei L-W
- Weinert M
- Weinstein AJ
- Weiss R
- Welborn T
- Wen L
- Westphal T
- Wette K
- Weßels P
- Whelan JT
- White DJ
- Whiting BF
- Williams RD
- Williamson AR
- Willis JL
- Willke B
- Wimmer MH
- Winkler W
- Wipf CC
- Wittel H
- Woan G
- Worden J
- Wright JL
- Wu G
- Yablon J
- Yam W
- Yamamoto H
- Yancey CC
- Yap MJ
- Yu H
- Yvert M
- Zadrożny A
- Zangrando L
- Zanolin M
- Zendri J-P
- Zevin M
- Zhang F
- Zhang L
- Zhang M
- Zhang Y
- Zhao C
- Zhou M
- Zhou Z
- Zhu XJ
- Zucker ME
- Zuraw SE
- Zweizig J
- Publication venue
- Living Rev Relativ
- Publication date
- 28/09/2021
- Field of study
We present a possible observing scenario for the Advanced LIGO and Advanced Virgo gravitational-wave detectors over the next decade, with the intention of providing information to the astronomy community to facilitate planning for multi-messenger astronomy with gravitational waves. We determine the expected sensitivity of the network to transient gravitational-wave signals, and study the capability of the network to determine the sky location of the source. We report our findings for gravitational-wave transients, with particular focus on gravitational-wave signals from the inspiral of binary neutron-star systems, which are considered the most promising for multi-messenger astronomy. The ability to localize the sources of the detected signals depends on the geographical distribution of the detectors and their relative sensitivity, and 90% credible regions can be as large as thousands of square degrees when only two sensitive detectors are operational. Determining the sky position of a significant fraction of detected signals to areas of 5 deg2 to 20 deg2 will require at least three detectors of sensitivity within a factor of ∼ 2 of each other and with a broad frequency bandwidth. Should the third LIGO detector be relocated to India as expected, a significant fraction of gravitational-wave signals will be localized to a few square degrees by gravitational-wave observations alone
Search for Gravitational Waves Associated with Gamma-Ray Bursts during the First Advanced LIGO Observing Run and Implications for the Origin of GRB 150906B
- Author
- Abbott BP
- Abbott R
- Abbott TD
- Abernathy MR
- Acernese F
- Ackley K
- Adams C
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Allen B
- Allocca A
- Altin PA
- Alvarez MD
- Ananyeva A
- Anderson SB
- Anderson WG
- Appert S
- Aptekar RL
- Arai K
- Araya MC
- Areeda JS
- Arnaud N
- Arun KG
- Ascenzi S
- Ashton G
- Ast M
- Aston SM
- Astone P
- Aufmuth P
- Aulbert C
- Avila-Alvarez A
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- Worden J
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- Yancey CC
- Yap MJ
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- Zadrozny A
- Zadrozny A
- Zangrando L
- Zanolin M
- Zendri J-P
- Zevin M
- Zhang L
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- Zhang T
- Zhang X
- Zhang Y
- Zhao C
- Zhou M
- Zhou Z
- Zhu XJ
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 29/11/2016
- Field of study
We present the results of the search for gravitational waves (GWs) associated with γ-ray bursts detected during the first observing run of the Advanced Laser Interferometer Gravitational-Wave Observatory (LIGO). We find no evidence of a GW signal for any of the 41 γ-ray bursts for which LIGO data are available with sufficient duration. For all γ-ray bursts, we place lower bounds on the distance to the source using the optimistic assumption that GWs with an energy of 10−2M⊙c2 were emitted within the 16–500 Hz band, and we find a median 90% confidence limit of 71 Mpc at 150 Hz. For the subset of 19 short/hard γ-ray bursts, we place lower bounds on distance with a median 90% confidence limit of 90 Mpc for binary neutron star (BNS) coalescences, and 150 and 139 Mpc for neutron star–black hole coalescences with spins aligned to the orbital angular momentum and in a generic configuration, respectively. These are the highest distance limits ever achieved by GW searches. We also discuss in detail the results of the search for GWs associated with GRB 150906B, an event that was localized by the InterPlanetary Network near the local galaxy NGC 3313, which is at a luminosity distance of 54 Mpc (z = 0.0124). Assuming the γ-ray emission is beamed with a jet half-opening angle ⩽30∘, we exclude a BNS and a neutron star–black hole in NGC 3313 as the progenitor of this event with confidence >99%. Further, we exclude such progenitors up to a distance of 102 Mpc and 170 Mpc, respectively
Observation of Gravitational Waves from a Binary Black Hole Merger
- Author
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- DeSalvo R
- Dhurandhar S
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- Zweizig J
- Publication venue
- American Physical Society
- Publication date
- 01/01/2016
- Field of study
On September 14, 2015 at 09:50:45 UTC the two detectors of the Laser Interferometer Gravitational-Wave
Observatory simultaneously observed a transient gravitational-wave signal. The signal sweeps upwards in
frequency from 35 to 250 Hz with a peak gravitational-wave strain of 1.0 × 10−21. It matches the waveform
predicted by general relativity for the inspiral and merger of a pair of black holes and the ringdown of the
resulting single black hole. The signal was observed with a matched-filter signal-to-noise ratio of 24 and a
false alarm rate estimated to be less than 1 event per 203 000 years, equivalent to a significance greater
than 5.1σ. The source lies at a luminosity distance of 410þ160
−180 Mpc corresponding to a redshift z ¼ 0.09þ0.03 −0.04 .
In the source frame, the initial black hole masses are 36þ5
−4M⊙ and 29þ4
−4M⊙, and the final black hole mass is
62þ4
−4M⊙, with 3.0þ0.5 −0.5M⊙c2 radiated in gravitational waves. All uncertainties define 90% credible intervals.
These observations demonstrate the existence of binary stellar-mass black hole systems. This is the first direct
detection of gravitational waves and the first observation of a binary black hole merger
Observation of gravitational waves from the coalescence of a 2.5−4.5 M⊙ compact object and a neutron star
- Author
- Abac Adrian
- Abbott R.
- Abouelfettouh I.
- Acernese F.
- Ackley Kendall
- Adhicary S.
- Adhikari Naresh
- Adhikari Rana X.
- Adkins V. K.
- Afif Ismail M.
- Agarwal Deepali
- Agathos Michalis
- Aghaei Abchouyeh Maryam
- Aguiar Odylio D.
- Aguilar I.
- Aiello Lorenzo
- Ain Anirban
- Ajith Parameswaran
- Akcay Sarp
- Akseli Hannuksela Otto
- Akutsu Tomotada
- Al-Jodah Ammar
- Al-Shammari S.
- Albanesi Simone
- Alex iandolo Guido
- Alfaidi Reem Atallah E
- Allocca Annalisa
- Alléné C.
- Altin Paul
- Alvarez-Lopez Sofia
- Amato Alex
- Amez-Droz L.
- Amorosi A.
- Amra C.
- Ananyeva A.
- Anderson Stuart
- Anderson Warren G.
- Andia Manuel
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- Andrade T.
- Andrea Prodi Giovanni
- Andres Nicolas
- Andric Tomislav
- Andrés Vallejo Peña Sergio
- Andrés-Carcasona Marc
- Anglin J.
- Anne Bizouard Marie
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- Antier Sarah
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- Zweizig John
- Árpád Gergely László
- 劉 國欽
- 都丸 隆行
- Publication venue
- Publication date
- 23/04/2024
- Field of study