121 research outputs found
Molecular mechanisms of EGF signaling-dependent regulation of pipe, a gene crucial for dorsoventral axis formation in Drosophila
- Author
- A Baonza
- A Shmueli
- A Siepel
- AC Spradling
- AH Tang
- AJ Courey
- AJ Whitmarsh
- AL Fisher
- AM Morimoto
- AM Queenan
- AS Tseng
- B Morgenstern
- B Morgenstern
- B Moussian
- BV Shravage
- C Ghiglione
- C Klambt
- C Pizzi
- C Xu
- CS Hill
- D Brunner
- D Morisato
- D Read
- D Read
- D Zhao
- DJ Goff
- DN Arnosti
- DS Latchman
- E Cinnamon
- EK LeMosy
- EM O'Neill
- EY Mantrova
- F Peri
- F Peri
- F Roch
- FS Neuman-Silberberg
- G Chen
- G Chinnadurai
- G Jimenez
- G Pavesi
- G Poortinga
- G Thijs
- G Thijs
- GV Flores
- J Sen
- J Zhu
- JB Duffy
- JD Hughes
- JD Thompson
- JD Wasserman
- JF Boisclair Lachance
- JJ Zartman
- JL Brown
- JV Price
- K Gaston
- KA Wharton Jr
- KC Jordan
- KE James
- L Fairall
- L Gabay
- LA Goentoro
- LA Nilson
- LM Pai
- M Blanchette
- M Blanchette
- M Blanchette
- M Buscarlet
- M Dissing
- M Fang
- M Kobayashi
- M Kobayashi
- M Mannervik
- M Rohrbaugh
- M Sutrias-Grau
- Martin Technau
- Meike Knispel
- MJ Shea
- MM Kulkarni
- MM Kulkarni
- MR Atkey
- MS Halfon
- N Bray
- N Yakoby
- NA Shevchuk
- O Couronne
- P Hasson
- P Hasson
- P Mani-Telang
- P Sergeev
- PP Tolias
- PP Tolias
- R Benezra
- R Lin
- R Treisman
- RL French
- S Astigarraga
- S Barolo
- S Gray
- S Gray
- S Gray
- S Li
- S Mahony
- S Mahony
- S Payankaulam
- S Roth
- S Roth
- S Roth
- SD Harrison
- Siegfried Roth
- SL McKnight
- SM Parkhurst
- T Hindemitt
- T Hsu
- T Hsu
- T Hsu
- T Hsu
- T Hunter
- T Xu
- TL Bailey
- TL Bailey
- TL Tootle
- WC Xiong
- WJ Kent
- WJ Kent
- WL Chang
- Y Nibu
- Y Wen
- YD Chung
- YS Cho
- Z Zhang
- Z Zhang
- ZC Lai
- ZC Lai
- ZC Lai
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2011
- Field of study
During Drosophila oogenesis the expression of the sulfotransferase Pipe in ventral follicle cells is crucial for dorsoventral axis formation. Pipe modifies proteins that are incorporated in the ventral eggshell and activate Toll signaling which in turn initiates embryonic dorsoventral patterning. Ventral pipe expression is the result of an oocyte-derived EGF signal which down-regulates pipe in dorsal follicle cells. The analysis of mutant follicle cell clones reveals that none of the transcription factors known to act downstream of EGF signaling in Drosophila is required or sufficient for pipe regulation. However, the pipe cis-regulatory region harbors a 31-bp element which is essential for pipe repression, and ovarian extracts contain a protein that binds this element. Thus, EGF signaling does not act by down-regulating an activator of pipe as previously suggested but rather by activating a repressor. Surprisingly, this repressor acts independent of the common co-repressors Groucho or CtBP
Multi-messenger observations of a binary neutron star merger
- Author
- Aab A
- Aartsen MG
- Abbott BP
- Abbott R
- Abbott TD
- Abbott TMC
- Abdalla H
- Abe F
- Abeysekara AU
- Abramo LR
- Abramowski A
- Abreu P
- Acernese F
- Acero F
- Ackermann M
- Ackley K
- Ackley K
- Adams C
- Adams J
- Adams SM
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Afrough M
- Agarwal B
- Agathos M
- Agatsuma K
- Aggarwal N
- Aglietta M
- Agliozzo C
- Agudo I
- Aguiar OD
- Aguilar JA
- Aharonian F
- Ahlers M
- Ahrens M
- Aiello L
- Ain A
- Ajith P
- Akras S
- Al Samarai I
- Albert A
- Albert A
- Albuquerque IFM
- Albury JM
- Alcaniz JS
- Alexander KD
- Alfaro R
- Alighieri S Di Serego
- Allam S
- Allekotte I
- Allen B
- Allen G
- Allison J
- Allison JR
- Allocca A
- Almela A
- Altin PA
- Altmann D
- Alvarez C
- Alvarez JD
- Alvarez M Dovale
- Alvarez-Muiz J
- Amati L
- Amato A
- An T
- Ananyeva A
- Anastasi GA
- Anchordoqui L
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- Zhang T
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- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Y-H
- Zhang YF
- Zhang YJ
- Zhang Z
- Zhang ZL
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- Zhao W
- Zhao XF
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- Zucker ME
- Zuniga J
- Zweizig J
- Zywucka N
- 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
Measurement of b hadron lifetimes in exclusive decays containing a J/psi in p-pbar collisions at sqrt(s)=1.96TeV
- Author
- Aaltonen T
- Gonzalez BA
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Badgett W
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Bland KR
- Blocker C
- Blumenfeld B
- Bocci A
- Bodek A
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Cabrera S
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung WH
- Chung YS
- Ciobanu CI
- Ciocci MA
- Clark A
- Clark D
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cox CA
- Cox DJ
- Crescioli F
- Almenar CC
- Cuevas J
- Culbertson R
- Dagenhart D
- d'Ascenzo N
- Datta M
- de Barbaro P
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- Deluca C
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- Deng J
- Deninno M
- Devoto F
- d'Errico M
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- Di Ruzza B
- Dittmann JR
- D'Onofrio M
- Donati S
- Dong P
- Dorigo T
- Ebina K
- Elagin A
- Eppig A
- Erbacher R
- Errede D
- Errede S
- Ershaidat N
- Eusebi R
- Fang HC
- Farrington S
- Feindt M
- Fernandez JP
- Ferrazza C
- Field R
- Flanagan G
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Furic I
- Gallinaro M
- Galyardt J
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerchtein E
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Ginsburg CM
- Giokaris N
- Giromini P
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- Golossanov A
- Gomez G
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- Goncharov M
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- Gorelov I
- Goshaw AT
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- Gresele A
- Grinstein S
- Grosso-Pilcher C
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- Haber C
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- Halkiadakis E
- Hamaguchi A
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- Scuri F
- Sedov A
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- Saulson PR
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- Summerscales TZ
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- Vahlbruch H
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- Vajente G
- Vallisneri M
- van den Brand JFJ
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- van der Putten S
- van der Sluys MV
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- Westphal T
- Wette K
- Whelan JT
- Whitcomb SE
- White D
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- Wilkinson C
- Willems PA
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- Willke B
- Winkelmann L
- Winkler W
- Wipf CC
- Wiseman AG
- Woan G
- Wooley R
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- Yakushin I
- Yamamoto H
- Yamamoto K
- Yeaton-Massey D
- Yoshida S
- Yu P
- Yvert M
- Zanolin M
- Zhang L
- Zhang Z
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- Zotov N
- Zucker ME
- Zweizig J
- Publication venue
- Publication date
- 01/12/2010
- Field of study
We report on a measurement of b-hadron lifetimes in the fully reconstructed
decay modes B^+ -->J/Psi K+, B^0 --> J/Psi K*, B^0 --> J/Psi Ks, and Lambda_b
--> J/Psi Lambda using data corresponding to an integrated luminosity of 4.3
fb−1, collected by the CDF II detector at the Fermilab Tevatron. The
measured lifetimes are τB^+ = 1.639±0.009(stat)±0.009(syst) ps, τB^0 = 1.507±0.010(stat)±0.008(syst) ps and τLambda_b = 1.537±0.045(stat)±0.014(syst) ps. The lifetime ratios are τB^+/τB^0 = 1.088±0.009(stat)±0.004(syst) and τLambda_b/τB^0 = 1.020±0.030(stat)±0.008(syst). These are the most precise determinations
of these quantities from a single experiment.Comment: revised version. accepted for PRL publicatio
Measurement of ZZ production in leptonic final states at {\surd}s of 1.96 TeV at CDF
- Author
- Aaltonen T.
- Alvarez Gonzalez B.
- Amerio S.
- Amidei D.
- Anastassov A.
- Annovi A.
- Antos J.
- Apollinari G.
- Appel J. A.
- Aptekar RL
- Arisawa T.
- Artikov A.
- Asaadi J.
- Ashmanskas W.
- Auerbach B.
- Aurisano A.
- Azfar F.
- Badgett W.
- Bae T.
- Barbaro-Galtieri A.
- Barnes V. E.
- Barnett B. A.
- Barria P.
- Bartos P.
- Bauce M.
- Bedeschi F.
- Behari S.
- Bellettini G.
- Bellinger J.
- Benjamin D.
- Beretvas A.
- Bhatti A.
- Bisello D.
- Bizjak I.
- Bland K. R.
- Blumenfeld B.
- Bocci A.
- Bodek A.
- Bortoletto D.
- Boudreau J.
- Boveia A.
- Boynton WV
- Briggs MS
- Brigliadori L.
- Bromberg C.
- Brucken E.
- Budagov J.
- Budd H. S.
- Burkett K.
- Busetto G.
- Bussey P.
- Buzatu A.
- Calamba A.
- Calancha C.
- Camarda S.
- Campanelli M.
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- Canelli F.
- Carls B.
- Carlsmith D.
- Carosi R.
- Carrillo S.
- Carron S.
- Casal B.
- Casarsa M.
- Castro A.
- Catastini P.
- Cauz D.
- Cavaliere V.
- Cavalli-Sforza M.
- Cerri A.
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- Chertok M.
- Chiarelli G.
- Chlachidze G.
- Chlebana F.
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- Chung W. H.
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- Connaughton V
- Convery M. E.
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- Crescioli F.
- Cuevas J.
- Culbertson R.
- d'Ascenzo N.
- d'Errico M.
- D'Onofrio M.
- da Costa J. Guimaraes
- Dagenhart D.
- Datta M.
- de Barbaro P.
- Dell'Orso M.
- Demortier L.
- Deninno M.
- Devoto F.
- Di Canto A.
- Di Ruzza B.
- Dittmann J. R.
- Donati S
- Dong P.
- Dorigo M.
- Dorigo T.
- Ebina K.
- Elagin A.
- Eppig A.
- Erbacher R.
- Errede S.
- Ershaidat N.
- Eusebi R.
- Farrington S.
- Feindt M.
- Fernandez J. P.
- Fernandez P. Movilla
- Field R.
- Flanagan G.
- Forrest R.
- Frank M. J.
- Franklin M.
- Frederiks DD
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- Furic I.
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- Giagu S.
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- Gold M.
- Goldin D.
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- Goldsten JO
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- Golovin D
- Gomez G.
- Gomez-Ceballos G.
- Goncharov M.
- Gonzalez O.
- Gorelov I.
- Goshaw A. T.
- Goulianos K.
- Grinstein S.
- Griso S. Pagan
- Grosso-Pilcher C.
- Group R. C.
- Hahn S. R.
- Halkiadakis E.
- Hamaguchi A.
- Han J. Y.
- Happacher F.
- Hara K.
- Hare D.
- Hare M.
- Harr R. F.
- Hatakeyama K.
- Hays C.
- Heck M.
- Heinrich J.
- Herndon M.
- Hewamanage S.
- Hocker A.
- Hopkins W.
- Horn D.
- Hou S.
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- Hurley KC
- Hurwitz M.
- Husemann U.
- Hussain N.
- Hussein M.
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- Introzzi G.
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- Ketchum W.
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- Knoepfel K.
- Kondo K.
- Kong D. J.
- Konigsberg J.
- Kotwal A. V.
- Kouveliotou C
- Kreps M.
- Krimm HA
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- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2011
- Field of study
In this paper we present a precise measurement of the total ZZ production
cross section in pp collisions at {\surd}s= 1.96 TeV, using data collected with
the CDF II detector corresponding to an integrated luminosity of approximately
6 fb-1. The result is obtained by combining separate measurements in the
four-charged (lll'l'), and two-charged-lepton and two-neutral-lepton (llvv)
decay modes of the Z. The combined measured cross section for pp {\to} ZZ is
1.64^(+0.44)_(-0.38) pb. This is the most precise measurement of the ZZ
production cross section in 1.96 TeV pp collisions to date.Comment: submitted to Phys. Rev. Let
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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- 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
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, 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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- Yamamoto Kazuhiro
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- Yamamoto T
- Yamashita K
- Yamazaki R
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- Yang Z
- Yap MJ
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- Yelikar AB
- Ying M
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- Yokozawa T
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- Yuzurihara H
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- Zanolin M
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- Zevin M
- Zhan M
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- 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
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: GW170817 and GRB 170817A
- Author
- Abbott BP
- Abbott R
- Abbott TD
- Acernese F
- Ackley K
- Adams C
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Afrough M
- Agarwal B
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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
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
- Ansoldi S
- Antelis JM
- Antier S
- Appert S
- Arai Koji
- Arai Koya
- Arai Y
- Araki S
- Araya A
- Araya MC
- Areeda JS
- Arellano FE Pena
- Arene M
- Aritomi N
- Arnaud N
- Aronson SM
- Asada H
- Asali Y
- Ashton G
- Aso Y
- Aston SM
- Astone P
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- Sipala V
- Skliris V
- Slagmolen BJJ
- Slaven-Blair TJ
- Smetana J
- Smith JR
- Smith RJE
- Somala SN
- Somiya K
- Son EJ
- Soni K
- Soni S
- Sorazu B
- Sordini V
- Sorrentino F
- Sorrentino N
- Sotani H
- Soulard R
- Souradeep T
- Sowell E
- Spagnuolo V
- Spencer AP
- Spera M
- Srivastava AK
- Srivastava V
- Staats K
- Stachie C
- Steer DA
- Steinlechner J
- Steinlechner S
- Stops DJ
- Stover M
- Strain KA
- Strang LC
- Stratta G
- Strunk A
- Sturani R
- Stuver AL
- Sudhagar S
- Sudhir V
- Suedbeck J
- Sugimoto R
- Suh HG
- Summerscales TZ
- Sun H
- Sun L
- Sunil S
- Sur A
- Suresh J
- Sutton PJ
- Suzuki Takamasa
- Suzuki Toshikazu
- Swinkels BL
- Szewczyk P
- Tacca M
- Tagoshi H
- Tait SC
- Takahashi H
- Takahashi R
- Takamori A
- Takano S
- Takeda H
- Takeda M
- Talbot C
- Tanaka H
- Tanaka Kazuyuki
- Tanaka Kenta
- Tanaka Taiki
- Tanaka Takahiro
- Tanasijczuk AJ
- Tanioka S
- Tanner DB
- Tao D
- Tapia A
- Tasson JD
- Telada S
- Tenorio R
- Terkowski L
- Test M
- Thirugnanasambandam MP
- Thomas M
- Thomas P
- Thompson JE
- Thondapu SR
- Thorne KA
- Thrane E
- Tiwari Shubhanshu
- Tiwari Srishti
- Tiwari V
- Toland K
- Tolley AE
- Tomaru T
- Tomigami Y
- Tomura T
- Tonelli M
- Torres-Forne A
- Torrie C
- Toyra D
- Trapananti A
- Travasso F
- Traylor G
- Tringali MC
- Tripathee A
- Troiano L
- 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
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- 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
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