104 research outputs found
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
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Allen B
- Allen G
- Allocca A
- Aloy MA
- Altin PA
- Alvarez MD
- Amato A
- Ananyeva A
- Anderson SB
- Anderson WG
- Angelova SV
- Antier S
- Appert S
- Arai K
- Araya MC
- Areeda JS
- Arnaud N
- Arun KG
- Ascenzi S
- Ashton G
- Ast M
- Aston SM
- Astone P
- Atallah DV
- Aufmuth P
- Aulbert C
- AultONeal K
- Austin C
- Avila-Alvarez A
- Babak S
- Bacon P
- Bader MKM
- Bae S
- Baker PT
- Baldaccini F
- Ballardin G
- Ballmer SW
- Banagiri S
- Barayoga JC
- Barclay SE
- Barish BC
- Barker D
- Barkett K
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Bartos I
- Bassiri R
- Basti A
- Batch JC
- Bawaj M
- Bayley JC
- Bazzan M
- Bazzano A
- Becsy B
- Beer C
- Bejger M
- Belahcene I
- Bell AS
- Berger BK
- Bergmann G
- Bero JJ
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- Bhagwat S
- Bhandare R
- Bilenko IA
- Billingsley G
- Billman CR
- Birch J
- Birney R
- Birnholtz O
- Biscans S
- Biscoveanu S
- Bisht A
- Bissaldi E
- Bitossi M
- Biwer C
- Bizouard MA
- Blackburn JK
- Blackburn L
- Blackman J
- Blair CD
- Blair DG
- Blair RM
- Bloemen S
- Bock O
- Bode N
- Boer M
- Bogaert G
- Bohe A
- Bondu F
- Bonilla E
- Bonnand R
- Boom BA
- Bork R
- Boschi V
- Bose S
- Bossie K
- Bouffanais Y
- Bozzi A
- Bozzo E
- Bradaschia C
- Brady PR
- Branchesi M
- Brandt S
- Brau JE
- Briant T
- Briggs MS
- Brillet A
- Brinkmann M
- Brisson V
- Brockill P
- Broida JE
- Brooks AF
- Brown DA
- Brown DD
- Brunett S
- Buchanan CC
- Buikema A
- Bulik T
- Bulten HJ
- Buonanno A
- Burns E
- Buskulic D
- Bustillo JC
- Buy C
- Byer RL
- Cabero M
- Cadonati L
- Cagnoli G
- Cahillane C
- Callister TA
- Calloni E
- Camp JB
- Canepa M
- Canizares P
- Cannon KC
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- Cerretani G
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- Chatziioannou K
- Cheeseboro BD
- Chen HY
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- Chen Y
- Chenevez J
- Cheng H-P
- Chia H
- Chincarini A
- Chiummo A
- Chmiel T
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- Chow JH
- Christensen N
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- Chua AJK
- Chua S
- Chung AKW
- Chung S
- Ciani G
- Ciolfi R
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- Cirone A
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- Cohen D
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- Connaughton V
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- Cooper SJ
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- Cordero-Carrion I
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- Etienne ZB
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- Frolov VV
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- Gadre BU
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- Ganija MR
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- Germain V
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- Zanolin M
- Zelenova T
- Zendri J-P
- Zertuche LM
- Zevin M
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- Zhou Z
- Zhu SJ
- Zhu XJ
- 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 5.0Ă10â8. 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 â3Ă10â15 and +7Ă10â16 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
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
- Abbott Bp
- Abbott R
- Abbott Td
- Abraham S
- Acernese F
- Ackley K
- Adams C
- Adhikari Rx
- Adya Vb
- Affeldt C
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar Od
- Aiello L
- Ain A
- Ajith P
- Allen G
- Allocca A
- Aloy Ma
- Altin Pa
- Amato A
- Anand S
- Ananyeva A
- Anderson Sb
- Anderson Wg
- Angelova Sv
- Antier S
- Appert S
- Arai K
- Araya Mc
- Areeda Js
- Arene M
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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%=3.47Ă10-25 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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- Araya Mc
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- Arene M
- Arnaud N
- Aronson Sm
- Ascenzi S
- Ashton G
- Aston Sm
- Astone P
- Aubin F
- Aufmuth P
- AultONeal K
- Austin C
- Avendano V
- Avila-Alvarez A
- Babak S
- Bacon P
- Badaracco F
- Bader Mkm
- Bae S
- Baird J
- Baker Pt
- Baldaccini F
- Ballardin G
- Ballmer Sw
- Bals A
- Banagiri S
- Barayoga Jc
- Barbieri C
- Barclay Se
- Barish Bc
- Barker D
- Barkett K
- Barnum S
- Barone F
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- Willke B
- Winkler W
- Wipf Cc
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- Woehler J
- Wofford Jk
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- Wu Ds
- Wysocki Dm
- Xiao S
- Xu R
- Yamamoto H
- Yancey Cc
- Yang L
- Yang Y
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- Zadrozny A
- Zadrozny Ak
- Zanolin M
- Zelenova T
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- Zhao G
- Zhou M
- Zhou Z
- Zhu Xj
- 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 LIGOâs 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=3.47Ă10â25 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
Charged-particle distributions at low transverse momentum in âs=13 13 TeV pp interactions measured with the ATLAS detector at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alstaty M
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Aranda CP
- Araque JP
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Measurements of distributions of charged particles produced in protonâproton collisions with a centre-of-mass energy of 13 TeV are presented. The data were recorded by the ATLAS detector at the LHC and correspond to an integrated luminosity of 151 ÎŒb â1 ÎŒbâ1 . The particles are required to have a transverse momentum greater than 100 MeV and an absolute pseudorapidity less than 2.5. The charged-particle multiplicity, its dependence on transverse momentum and pseudorapidity and the dependence of the mean transverse momentum on multiplicity are measured in events containing at least two charged particles satisfying the above kinematic criteria. The results are corrected for detector effects and compared to the predictions from several Monte Carlo event generators
Search for dark matter at âs=13 TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector
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- Zhemchugov A
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
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- Zou R
- Zu Theenhausena HM
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fbâ1 of protonâproton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, model-independent limits are set on the fiducial cross section for the production of events in this final state. Exclusion limits are also placed in models where dark-matter candidates are pair-produced. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750â1200 GeV for dark-matter candidate masses below 230â480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale Mâ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to ZÎł and the Z boson subsequently decays into neutrinos
Measurement of W+Wâ production in association with one jet in protonâproton collisions at sqrt(s) = 8TeV with the ATLAS detector
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- Rimoldi A
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- Ristic B
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- Robinson JEM
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- Schmitt C
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- Schoening A
- Schoenrock BD
- Schopf E
- Schott M
- Schouwenberg JFP
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- Schramm S
- Schreyer M
- Schroeder TV
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- Schultens MJ
- Schultz-Coulon H-C
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- Schune P
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- Schweiger H
- Schwemling P
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- Sciolla G
- Scuri F
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- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shaikh NW
- Shan LY
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- Shatalov PB
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- Shehu CY
- Sherwood P
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- Shimmin CO
- Shimojima M
- Shirabe S
- Shiyakova M
- Shmeleva A
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- Shojaii S
- Shope DR
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
- Sickles AM
- Sidebo PE
- Sidiropoulou O
- Sidorov D
- Sidoti A
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- Silverstein SB
- Simak V
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- Sinervo P
- Sinev NB
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- Siragusa G
- Sivoklokov SY
- Sjolin J
- Skinner MB
- Skottowe HP
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smestad L
- Smiesko J
- Smirnov SY
- Smirnov Y
- Smirnova LN
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- Smizanska M
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- Soffer A
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- Sokhrannyi G
- Sola JDB
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- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
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- Song HY
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- Sorin V
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- Sotiropoulou CL
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- Spighi R
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- Spiller LA
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- Stelzer HJ
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- Stewart GA
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- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strandlie A
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- Strubig A
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- Su D
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- Sumida T
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- Sundermann JE
- Suruliz K
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- Svatos M
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- Sykora I
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- Talyshev AA
- Tan KG
- Tanaka J
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- Tannenwald BB
- Tapprogge S
- Tarem S
- Tartarelli GF
- Tas P
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- Tashiro T
- Tassi E
- Tayalati Y
- Taylor AC
- Taylor GN
- Taylor PTE
- Taylor W
- Tehrani FS
- Teischinger FA
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- Temming KK
- Temple D
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
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- Terzo S
- Testa M
- Teuscher RJ
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- Thomsen LA
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- Tripiana MF
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- Trocme B
- Trofymov A
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- Truong L
- Trzebinski M
- Trzupek A
- Tseng JC-L
- Tsiareshka PV
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsui KM
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turgeman D
- Turra R
- Tuts PM
- Tyndel M
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Unverdorben C
- Urban J
- Urban SC
- Urquijo P
- Urrejola P
- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Valderanis C
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- Valentinetti S
- Valero A
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- Valkar S
- Van DenWollenberg W
- Van Der Deijl PC
- Van der Graaf H
- van Eldik N
- van Gemmeren P
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- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vanguri R
- Vaniachine A
- Vankov P
- Vardanyan G
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- Varnes EW
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- Veeraraghavan V
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- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Verzini MJA
- Vest A
- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Villa M
- Villar DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vittori C
- Vivarelli I
- Vlachos S
- Vlasak M
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
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- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
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- Wallangen V
- Walls FMG
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- Warburton A
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- Wardrope DR
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- Weber MS
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- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weiser C
- Weits H
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
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- White MJ
- White R
- Whiteson D
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- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wittkowski J
- Wolf TMH
- Wolter MW
- Wolters H
- Wong KHY
- Worm SD
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wu M
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yuen SPY
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeid OSA
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhangb H
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
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- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2016
- Field of study
The production of W boson pairs in association with one jet in pp collisions at View the MathML sources=8 TeV is studied using data corresponding to an integrated luminosity of 20.3 fbâ1 collected by the ATLAS detector during 2012 at the CERN Large Hadron Collider. The cross section is measured in a fiducial phase-space region defined by the presence of exactly one electron and one muon, missing transverse momentum and exactly one jet with a transverse momentum above 25 GeV and a pseudorapidity of |η|<4.5|η|<4.5. The leptons are required to have opposite electric charge and to pass transverse momentum and pseudorapidity requirements. The fiducial cross section is found to be View the MathML sourceÏWWfid,1-jet=136±6(stat)±14(syst)±3(lumi) fb. In combination with a previous measurement restricted to leptonic final states with no associated jets, the fiducial cross section of WW production with zero or one jet is measured to be View the MathML sourceÏWWfid,â€1-jet=511±9(stat)±26(syst)±10(lumi) fb. The ratio of fiducial cross sections in final states with one and zero jets is determined to be 0.36±0.050.36±0.05. Finally, a total cross section extrapolated from the fiducial measurement of WW production with zero or one associated jet is reported. The measurements are compared to theoretical predictions and found in good agreement
Localization and broadband follow-up of the gravitational-wave transient GW150914
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- Zweizig J
- 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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- Moore CJ
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- Moskalenko IV
- Moskvitin AS
- Mostaf M
- Motohara K
- Moulai M
- Moulin E
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- Moussa A
- Mow-Lowry CM
- Mrka S
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- Mueller G
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- Mueller S
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- Mukherjee D
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- Mundell CG
- Muniz EA
- Muoz A Gonzolez
- Muoz RR
- Murach T
- Murata KL
- Muratore M
- Murguia-Berthier A
- Murphy T
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- Nagai H
- Nagashima H
- Nagayama T
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- Nakahira S
- Nakajima M
- Nakamura Y
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- Ngeow C-C
- Nguyen P
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- Nie JY
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- Nielsen AB
- Niemiec J
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- Observat Toros Transient Robotic
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- Orlando E
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- Ostrowski M
- Ottaway DJ
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- Palamos JR
- Palashov O
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- Palazzi E
- Palczewski T
- Paliya VS
- Palliyaguru N
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- Palmerio JT
- Palmese A
- Palomba C
- Pan Howard
- Pan Huang-Wei
- 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
- Paoletti F
- Paoletti F
- Paoli A
- Papa MA
- Papenbreer P
- Paragi Z
- Parente G
- Parida A
- Park IH
- Parker W
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- Parmiggiani N
- Parra A
- Parsons RD
- Pascucci D
- Pasqualetti A
- Passaquieti R
- Passuello D
- Pastorello A
- Patat F
- Pathfinder ASKAP Australian SKA
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- Paul T
- Pavalas GE
- Pavana M
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- Paz-Chinchn F
- Pea-Rodriguez J
- Pearlstone BL
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- Pedraza M
- Pedreira F
- Pedurand R
- Peiffer P
- Peixoto CJ Todero
- Pekeur NW
- Pekowsky L
- Pelayo R
- Pele A
- Pellegrino C
- Pelletier G
- Pellizzoni A
- Penacchioni AV
- Penn S
- Penuela T
- Pepper JA
- Pereira LAS
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- Perez CJ
- Perez-Perez EG
- Perley DA
- Perlin M
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- Perri LM
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- Perrodin D
- Perrone L
- Pescalli A
- Pesce-Rollins M
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- Petrucci P-O
- Peyaud B
- Pfeiffer HP
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- Pian E
- Piano G
- Piattelli P
- 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
- Pittori C
- Placco VM
- Platino M
- Plazas AA
- Plum M
- Podesta F
- Podesta RC
- Podsiadlowski P
- Poe M
- Poggiani R
- Poh J
- Poireau V
- Pollmann A Obertacke
- Poolakkil S
- Poon H
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- Popolizio P
- Poppi S
- Porowski C
- Porter EK
- Porter TA
- Possenti A
- Post A
- Potter SB
- Powell J
- Pozanenko AS
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- Prado RR
- Prasad J
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- Prestegard T
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- Principe G
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- Prodi GA
- Prokhorov D
- Prokhorov LG
- Prokoph H
- Prouza M
- Prrer M
- Przybylski GT
- Pulone L
- Pumo ML
- Punch M
- Puncken O
- Punturo M
- Puppo P
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- Quataert E
- Quel EJ
- Querchfeld S
- Querel R
- Quetschke V
- Quimby RM
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- Quirrenbach A
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- Ramos-Buades A
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- RATIR RIMAS
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- Reid S
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- Reimer A
- Reimer O
- Reimer O
- Reitze DH
- Relethford B
- Relich M
- Ren W
- Ren Z
- Renaud M
- Renzi V
- Reposeur T
- Resconi E
- Resmi L
- Rest A
- Reva IV
- Reyes R De Los
- Reyes SD
- Reynolds T
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- Riviere C
- Rizi V
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- Robertson S
- Robie R
- Robinet F
- Rocchi A
- Rochester LS
- Rodi J
- Rodriguez H
- Rojas D Avila
- Rojas-Bravo C
- Rojo J Rodriguez
- Rol E
- Rolland L
- Rollins JG
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- Romano R
- Romel CL
- Romer AK
- Romero M Dominguez
- Romie JH
- Romoli C
- Roncoroni MJ
- Rongen M
- Roodman A
- Roques J-P
- Rosa-Gonzlez D
- Rosell A Carnero
- Rosenberg M
- Rosetti S
- Rosinska D
- Ross MP
- Rossi A
- Rosswog S
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- Roth M
- Rott C
- Roulet E
- Rovero AC
- Rowan S
- Rowell G
- Rowlinson A
- Rowlinson A
- Roy R
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- Rudak B
- Ruehl P
- Ruggi P
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- Ruiz R Gracia
- Ruiz-Velasco E
- Rulten CB
- Rumyantsev VV
- Rusu F
- Rutins G
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- Ryckbosch D
- Rykoff ES
- Rysewyk D
- Saba A
- Sachdev S
- Sadecki T
- Sadeghian L
- Sadler EM
- Sadler EM
- Saffe C
- Saffi SJ
- Saftoiu A
- Sahakian V
- Sai N
- Saito S
- Saito T
- Saito Y
- Sakamaki A
- Sakamoto T
- Sakellariadou M
- Sako M
- Sako S
- Salafia OS
- Salamida F
- Salazar H
- Salazar H
- Salconi L
- Saldaa M
- Saleem M
- Saleh A
- Salemi F
- Salina G
- Salmon L
- 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
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- Sanchez-Lucas P
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- Sanchis-Gual N
- Sand DJ
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- Sandrock A
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- Sansom EK
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- Santangelo A
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- Sarazin F
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- Sasaki M
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- Satalecka K
- Sathyaprakash BS
- Sato R
- Saulson PR
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- Sauter O
- Savage RL
- Savchenko V
- Sawadsky A
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- Schmidt J
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- Schoenell W
- Schoenen S
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- Schonbeck A
- Schoneberg S
- Schoorlemmer H
- Schovnek P
- Schreiber E
- Schroder FG
- Schroder S
- Schroder SL
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- Schuette D
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- Schultz ASB
- Schulz A
- Schulz A
- Schulze S
- Schumacher J
- Schumacher L
- Schutz BF
- Schwalbe SG
- Schwanke U
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- Schweyer T
- Sciutto SJ
- Scolnic D
- Scott J
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- Secco LF
- Seckel D
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- Segreto A
- Seidel E
- Seitenzahl IR
- Sekiguchi Y
- Sellers D
- Selsing J
- Sengupta AS
- Sentenac D
- Sequino V
- Sergeev A
- Sergienko Yu P
- Serino M
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- Seunarine S
- Sevilla-Noarbe I
- Seyffert AS
- Sgro C
- Shaddock DA
- Shadkam A
- Shaffer TJ
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- Shah AA
- Shahriar MS
- Shaner MB
- Shang Z
- Shannon RM
- Shao L
- Shapiro B
- Shappee BJ
- Shara MM
- Sharma I
- Sharp RG
- Shawhan P
- Sheldon E
- Shellard RC
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- Shilon I
- Shimizu Y
- Shimomukai R
- Shingles LJ
- Shiningayamwe K
- Shoemaker DH
- Shoemaker DM
- Shulevski A
- Siebert MR
- Siegel MH
- Sieger C
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- Siemens X
- Sieniawska M
- Sigg D
- Sigl G
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- Silva AD
- Sim SA
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- Simonetti JH
- Simoni R
- Singer LP
- Singh A
- Singhal A
- Sinnis G
- Sintes AM
- Siskind EJ
- Slagmolen BJJ
- Slzer T
- Smartt SJ
- Smida R
- Smirnov OM
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- Smith B
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- Smith KW
- Smith M
- Smith M
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- Snow GR
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- Sobreira F
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- Soedingrekso J
- Soffitta P
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- Sol H
- Solares HA Ayala
- Soldin D
- Sollerman J
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- Sorrentino F
- Souradeep T
- Spada F
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- Spanier F
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- Spiczak GM
- Spiering C
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- Springer RW
- Spurio M
- Squartini R
- Srivastava AK
- Staats K
- Stachurska J
- Staff J
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- Staley A
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- Stamerra A
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- Stanic S
- Stanway ER
- Starck M
- Starling RLC
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- Stasik A
- Stassi P
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- Steeghs DTH
- Steele I
- Steele K
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- Stewart AJ
- Stezelberger T
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- Stolarczyk Th
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- Stone R
- Stops DJ
- Stosl A
- Strafella F
- Strain KA
- Stratta G
- Streich A
- Strigin SE
- Strotjohann NL
- Strunk A
- Stubbs CW
- Sturani R
- Stuttard T
- Stuver AL
- Suarez F
- Suarez-Duran M
- Suchyta E
- Sudholz T
- Sugawara Y
- Sugita S
- Sugizaki M
- Sullivan GW
- Sullivan M
- Sumi T
- Summerscales TZ
- Sun L
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- Sun T
- Sunil S
- Suntzeff NB
- Sunyaev R
- Suomijarvi T
- Supanitsky AD
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- Surcis G
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- Suson DJ
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- Swanson MEC
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- Szomoru A
- Taboada A
- Taboada I
- Taborda OA
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- Tachibana Y
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- Takahashi I
- Takahashi J
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- Talbot C
- Talukder D
- Tamura T
- Tamura Y
- Tan Y
- Tanaka I
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- Tanner DB
- Tanvir NR
- Tao C
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- Tao WH
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- Tenholt F
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- Ter-Antonyan S
- Terai T
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- Terreran G
- Terrier R
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- Testa V
- Tewari SV
- Thayer JB
- Thayer JG
- Theeg T
- Thene CC
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- Thrane E
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- Tingay SJ
- Tiwari S
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- Tiziani D
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- Tokmakov KV
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- Tome B
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- Torresi E
- Torrie CI
- Toscano S
- Tosi D
- Towner MC
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- Tristram PJ
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- Troxel MA
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- Tsang KW
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- Tsirou M
- Tso R
- Tsuboi Y
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- Tsuna D
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- Tsvetkova AE
- Tucker BE
- Tucker DL
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- Tuffs R
- Tung CF
- Tungalag N
- Tuo YL
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- Turley CF
- Turpin D
- Turpin D
- Tuyenbayev D
- Ty B
- Tyurina NV
- Ubertini P
- Uchiyama Y
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- Ugolini D
- Ukwatta TN
- Ulaczyk K
- Ulanov MV
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- Ulrich R
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- Utsumi Y
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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 transientâs 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
A search for pair-produced resonances in four-jet final states at root s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
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- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
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- Zacharis G
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- Zalieckas J
- Zaman A
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- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
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- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
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- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 03/04/2017
- Field of study
A search for massive coloured resonances which are pair-produced and decay into two jets is presented. The analysis uses 36.7 fbâ1
â
1
of â
s
= 13 TeV pp collision data recorded by the ATLAS experiment at the LHC in 2015 and 2016. No significant deviation from the background prediction is observed. Results are interpreted in a SUSY simplified model where the lightest supersymmetric particle is the top squark, Ì
t
~
, which decays promptly into two quarks through R-parity-violating couplings. Top squarks with masses in the range 100 GeV<Ì<410
100
GeV
<
m
t
~
<
410
GeV
GeV
are excluded at 95% confidence level. If the decay is into a b-quark and a light quark, a dedicated selection requiring two b-tags is used to exclude masses in the ranges 100 GeV<Ì<470
100
GeV
<
m
t
~
<
470
GeV
GeV
and 480 GeV<Ì<610
480
GeV
<
m
t
~
<
610
GeV
GeV
. Additional limits are set on the pair-production of massive colour-octet resonances
Measurements of electroweak Wjj production and constraints on anomalous gauge couplings with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Alieva M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
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- Alshehri AA
- Alstaty M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Amelung C
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- Angelidakis S
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- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Measurements of the electroweak production of a W boson in association with two jets at high dijet invariant mass are performed using root s = 7 and 8 TeV proton-proton collision data produced by the Large Hadron Collider, corresponding respectively to 4.7 and 20.2 fb(-1) of integrated luminosity collected by the ATLAS detector. The measurements are sensitive to the production of a W boson via a triple-gauge-boson vertex and include both the fiducial and differential cross sections of the electroweak process
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