76 research outputs found
A MISSING-LINK IN THE SUPERNOVA-GRB CONNECTION: THE CASE OF SN 2012ap
- Author
- A. B. Sanin
- A. Rau
- A. von Kienlin
- Alak Ray
- Alicia Soderberg
- Andreas Brunthaler
- Andrew MacFadyen
- Atish Kamble
- Bietenholz M. F.
- C. Fellows
- Cenko S. B.
- Chakraborti S.
- Chevalier R. A.
- Chiang J.
- Claes Fransson
- Cornwell T.
- D. Frederiks
- D. Golovin
- D. Palmer
- D. Svinkin
- Dan Milisavljevic
- Elena Pian
- Emily Levesque
- Giuliano Pignata
- H. Enos
- H. Krimm
- Horesh A.
- Hurley K.
- I. G. Mitrofanov
- J. Cummings
- J. Goldsten
- Jason Dittmann
- Jewett L.
- K. Harshman
- K. Yamaoka
- Kevin Hurley
- Laura Chomiuk
- M. L. Litvak
- M. Ohno
- M. S. Briggs
- M. Tashiro
- Margutti R.
- Mario Hamuy
- Matzner C. D.
- Michael Bietenholz
- Milisavljevic D.
- Milisavljevic D.
- Milisavljevic D.
- Miriam Krauss
- N. Gehrels
- Naveen Yadav
- Norbert Bartel
- Nugis T.
- Pacholczyk A. G.
- Paolo Mazzali
- R. Aptekar
- Raffaella Margutti
- Ruderman M. ed Bergman P. G.
- Rybicki G. B.
- S. Barthelmy
- S. Golenetskii
- Sayan Chakraborti
- Springob C. M.
- T. Cline
- T. Murakami
- T. Takahashi
- V. Connaughton
- V. Savchenko
- W. Boynton
- X. Zhang
- Y. Fukazawa
- Y. Terada
- Publication venue
- 'IOP Publishing'
- Publication date
- 22/04/2015
- Field of study
Gamma Ray Bursts (GRBs) are characterized by ultra-relativistic outflows,
while supernovae are generally characterized by non-relativistic ejecta. GRB
afterglows decelerate rapidly usually within days, because their low-mass
ejecta rapidly sweep up a comparatively larger mass of circumstellar material.
However supernovae, with heavy ejecta, can be in nearly free expansion for
centuries. Supernovae were thought to have non-relativistic outflows except for
few relativistic ones accompanied by GRBs. This clear division was blurred by
SN 2009bb, the first supernova with a relativistic outflow without an observed
GRB. Yet the ejecta from SN 2009bb was baryon loaded, and in nearly-free
expansion for a year, unlike GRBs. We report the first supernova discovered
without a GRB, but with rapidly decelerating mildly relativistic ejecta, SN
2012ap. We discovered a bright and rapidly evolving radio counterpart driven by
the circumstellar interaction of the relativistic ejecta. However, we did not
find any coincident GRB with an isotropic fluence of more than a sixth of the
fluence from GRB 980425. This shows for the first time that central engines in
type Ic supernovae, even without an observed GRB, can produce both relativistic
and rapidly decelerating outflows like GRBs.Comment: 8 pages, 5 figures, 1 table, accepted for publication in Ap
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
- Adams C
- Adhikari RX
- 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
- Ando M
- Angelova S
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- Antelis JM
- Antier S
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- Arai Koji
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- Araki S
- Araya A
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- Areeda JS
- Arellano FE Pena
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- Aritomi N
- Arnaud N
- Aronson SM
- Asada H
- Asali Y
- Ashton G
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- Yamamoto Kazuhiro
- Yamamoto Kohei
- Yamamoto T
- Yamashita K
- Yamazaki R
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- Yang Yang
- Yang Yi
- Yang Z
- Yap MJ
- Yeeles DW
- Yelikar AB
- Ying M
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- Yu Hang
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- Zevin M
- Zhan M
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- 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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- 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
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
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- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- College Park, MD : American Physical Society
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO's second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h095%=3.47×10-25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering. © 2019 American Physical Society
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
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- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO’s second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h95%0=3.47×10−25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering
All-sky search for gravitational-wave bursts in the second joint LIGO-Virgo run
- Author
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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
GWTC-2.1: Deep extended catalog of compact binary coalescences observed by LIGO and Virgo during the first half of the third observing run
- Author
- Abbott R
- Abbott TD
- Acernese F
- Ackley K
- Adams C
- Adhikari N
- Adhikari RX
- Adya VB
- Affeldt C
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- Woan G
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- Wofford JK
- Wong ICF
- Wu DS
- Wysocki DM
- Xiao L
- Yamamoto H
- Yang FW
- Yang L
- Yang Yang
- Yang Z
- Yap MJ
- Yeeles DW
- Yelikar AB
- Ying M
- Yoo J
- Yu Hang
- Yu Haocun
- Zadrożny A
- Zanolin M
- Zelenova T
- Zendri J-P
- Zevin M
- Zhang J
- Zhang L
- Zhang T
- Zhang Y
- Zhao C
- Zhao G
- 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
Localization and broadband follow-up of the gravitational-wave transient GW150914
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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
Multi-messenger observations of a binary neutron star merger
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- Li MS
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- Li TP
- Li TS
- Li W
- Li X
- Li X
- Li XB
- Li XF
- Li YG
- Li ZJ
- Li ZW
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- Lidman C
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- Longinotti AL
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- Mazumder N
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- Nielsen AB
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- Observat Toros Transient Robotic
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- Pan Howard
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- Pan Y-C
- Pan-STARRS
- Pandey SB
- Pandya H
- Paneque D
- Pang B
- Pang PTH
- Pankova DV
- Pankow C
- Pannarale F
- Pant BC
- Panter M
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- Paoletti F
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- Parmiggiani N
- Parra A
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- Pascucci D
- Pasqualetti A
- Passaquieti R
- Passuello D
- Pastorello A
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- Pavalas GE
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- Pea-Rodriguez J
- Pearlstone BL
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- Peixoto CJ Todero
- Pekeur NW
- Pekowsky L
- Pelayo R
- Pele A
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- Peyaud B
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- Pian E
- Piano G
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- Piccinni OJ
- Pichot M
- Picozza P
- Piel Q
- Pieloth D
- Piergiovanni F
- Pierog T
- Pierro V
- Pignata G
- Pike S
- Pilia M
- Pillant G
- Pimenta M
- Pinard L
- Pinat E
- Pinto IM
- Piotrowski LW
- Piran T
- Piran T
- Piranomonte S
- Pirello M
- Piro AL
- Piro L
- Piron F
- Pirronello V
- Pisanu T
- Pita S
- Pitkin M
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- Placco VM
- Platino M
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- Podesta F
- Podesta RC
- Podsiadlowski P
- Poe M
- Poggiani R
- Poh J
- Poireau V
- Pollmann A Obertacke
- Poolakkil S
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- Popolizio P
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- Possenti A
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- Powell J
- Pozanenko AS
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- Prado RR
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- Pratt JWW
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- Price LR
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- Principe G
- Principe M
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- Privitera P
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- Prochaska JX
- Prodi GA
- Prokhorov D
- Prokhorov LG
- Prokoph H
- Prouza M
- Prrer M
- Przybylski GT
- Pulone L
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- Quimby RM
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- Ren Z
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- Reposeur T
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- Robie R
- Robinet F
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- Rochester LS
- Rodi J
- Rodriguez H
- Rojas D Avila
- Rojas-Bravo C
- Rojo J Rodriguez
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- Roma VJ
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- Romero M Dominguez
- Romie JH
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- Rosell A Carnero
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- Ruiz-Velasco E
- Rulten CB
- Rumyantsev VV
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- Sadler EM
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- Saffe C
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- Sahakian V
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- Saito Y
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- Sako M
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- Salafia OS
- Salamida F
- Salazar H
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- Salvadori I
- Salvaterra R
- Samajdar A
- Sammut L
- Sampedro L
- Sampson LM
- Samtleben DFE
- Sanchez B
- Sanchez DA
- Sanchez E
- Sanchez EJ
- Sanchez F
- Sanchez LE
- Sanchez-Losa A
- Sanchez-Lucas P
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- Sanchis-Gual N
- Sand DJ
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- Sanders JR
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- Santangelo A
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- Sarazin F
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- Sathyaprakash BS
- Sato R
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- Schmidt BP
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- Schneider A
- Schneider M
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- Schoenell W
- Schoenen S
- Schofield RMS
- Scholten O
- Schonbeck A
- Schoneberg S
- Schoorlemmer H
- Schovnek P
- Schreiber E
- Schroder FG
- Schroder S
- Schroder SL
- Schssler F
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- Schuette D
- Schulte BW
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- Schulz A
- Schulz A
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- Schwalbe SG
- Schwanke U
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- Sciutto SJ
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- Segreto A
- Seidel E
- Seitenzahl IR
- Sekiguchi Y
- Sellers D
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- Sengupta AS
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- Sergeev A
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- Seunarine S
- Sevilla-Noarbe I
- Seyffert AS
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- Shaffer TJ
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- Shah AA
- Shahriar MS
- Shaner MB
- Shang Z
- Shannon RM
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- Shara MM
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- Sharp RG
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- Shilon I
- Shimizu Y
- Shimomukai R
- Shingles LJ
- Shiningayamwe K
- Shoemaker DH
- Shoemaker DM
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- Siebert MR
- Siegel MH
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- Siemens X
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- Sintes AM
- Siskind EJ
- Slagmolen BJJ
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- Starling RLC
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- Strafella F
- Strain KA
- Stratta G
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- Strigin SE
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- Strunk A
- Stubbs CW
- Sturani R
- Stuttard T
- Stuver AL
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- Suchyta E
- Sudholz T
- Sugawara Y
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- Sullivan GW
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- Summerscales TZ
- Sun L
- Sun L
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- Sunil S
- Suntzeff NB
- Sunyaev R
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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
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: GW170817 and GRB 170817A
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- 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
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