398 research outputs found
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
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- Azuma Y
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- Backhaus M
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- Chekulaev SV
- Chelkov GA
- Chelstowska MA
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- Chen H
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- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
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- Chiefari G
- Chikovani L
- Childers JT
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- Chizhov MV
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
- Author
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- Yilmaz M
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- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenin O
- Zenis T
- Zerwas D
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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 23/11/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Z′ Models
Murine Models and Cell Lines for the Investigation of Pheochromocytoma: Applications for Future Therapies?
- Author
- A Besson
- A Cascon
- A Cristofano Di
- A Cristofano Di
- A Fritz
- A Shyla
- AG Knudson
- AM Senderowicz
- AP Gimenez-Roqueplo
- AS Tischler
- AY Nikitin
- BJ Petri
- CA Koch
- CJ Sherr
- DA Solomon
- DA Sweetser
- DL Burkhart
- DS Franklin
- DS Franklin
- DS Goldstein
- E Edstrom
- E Korpershoek
- Esther Korpershoek
- EW Lai
- F Bai
- F Nederveen van
- FH Nederveen van
- FM Brouwers
- G Eisenhofer
- G Eisenhofer
- H Dannenberg
- HJ Timmers
- HJ Timmers
- I Comino-Mendez
- I Marinoni
- ID Tonks
- J Lu
- J Sandgren
- J Wakai
- JC Sisson
- JC Sisson
- JC Sisson
- JF Powers
- JF Powers
- JF Powers
- JF Powers
- JF Powers
- JH Dannenberg
- JP Bayley
- JP Bayley
- JV Glowniak
- JW Lenders
- K Hansen
- K Kawakami
- K Pacak
- K Pacak
- Karel Pacak
- KC Loh
- L Martiniova
- L Martiniova
- L Martiniova
- L Martiniova
- L Martiniova
- L Martiniova
- L Yamasaki
- LQ Le
- Lucia Martiniova
- M Georgitsi
- M Zamanian
- MJ You
- MS Airaksinen
- MV Kulkarni
- N Dyson
- NE Sharpless
- NS Pellegata
- NS Pellegata
- P Bachireddy
- PL Dahia
- PL Dahia
- PP Joshi
- R Munver
- R Salgia
- RV Thakker
- S Courtois-Cox
- S Goncalves
- S Gratias
- S Hoegerle
- S Kunwar
- S Molatore
- S Ohta
- S Schlisio
- SD Averbuch
- T Jacks
- V Dhawan
- V Pachnis
- V Stambolic
- VC Williams
- W Lutz
- W Veelen van
- Y Kitamura
- Y Kitamura
- Y Qin
- YE Nikiforov
- Publication venue
- Springer US
- Publication date
- 01/01/2012
- Field of study
Pheochromocytomas (PCCs) are slow-growing neuroendocrine tumors arising from adrenal chromaffin cells. Tumors arising from extra-adrenal chromaffin cells are called paragangliomas. Metastases can occur up to approximately 60% or even more in specific subgroups of patients. There are still no well-established and clinically accepted “metastatic” markers available to determine whether a primary tumor is or will become malignant. Surgical resection is the most common treatment for non-metastatic PCCs, but no standard treatment/regimen is available for metastatic PCC. To investigate what kind of therapies are suitable for the treatment of metastatic PCC, animal models or cell lines are very useful. Over the last two decades, various mouse and rat models have been created presenting with PCC, which include models presenting tumors that are to a certain degree biochemically and/or molecularly similar to human PCC, and develop metastases. To be able to investigate which chemotherapeutic options could be useful for the treatment of metastatic PCC, cell lines such as mouse pheochromocytoma (MPC) and mouse tumor tissue (MTT) cells have been recently introduced and they both showed metastatic behavior. It appears these MPC and MTT cells are biochemically and molecularly similar to some human PCCs, are easily visualized by different imaging techniques, and respond to different therapies. These studies also indicate that some mouse models and both mouse PCC cell lines are suitable for testing new therapies for metastatic PCC
Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
- Author
- Aad G
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- Abdallah J
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- Abramowicz H
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5 fb[superscript −1] of proton-proton collisions data at √s=7 TeV and 20.3 fb[superscript −1] at √s=8 TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be μ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4 GeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m[subscript H]. They are found to be μ[subscript ggF]=1.32±0.38, μ[subscript VBF]=0.8±0.7, μ[subscript WH]=1.0±1.6, μ[subscript ZH]=0.1[superscript +3.7 subscript −0.1], and μ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript −1.8], for Higgs boson production through gluon fusion, vector-boson fusion, and in association with a W or Z boson or a top-quark pair, respectively. Compared with the previously published ATLAS analysis, the results reported here also benefit from a new energy calibration procedure for photons and the subsequent reduction of the systematic uncertainty on the diphoton mass resolution. No significant deviations from the predictions of the Standard Model are found.European Organization for Nuclear ResearchUnited States. Dept. of EnergyNational Science Foundation (U.S.)Brookhaven National Laborator
Measurement of W+W− production in association with one jet in proton–proton collisions at sqrt(s) = 8TeV with the ATLAS detector
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- Yildiz HD
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- Yoshihara K
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- Youssef S
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- Zalieckas J
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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhu CG
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
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- 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 fb−1 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 sourceσWWfid,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 sourceσWWfid,≤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
Charged-particle distributions at low transverse momentum in √s=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
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- 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
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
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- 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 proton–proton 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 μb −1 μb−1 . 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 the b(b)over-bar decay of the Standard Model Higgs boson in associated (W/Z)H production with the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
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Search for pair production of Higgs bosons in the bb¯bb¯ final state using proton-proton collisions at √s=13 TeV with the ATLAS detector
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- Meehan S
- Mehlhase S
- Mehta A
- Meier K
- Meineck C
- Meirose B
- Melini D
- Melo M
- Meloni F
- Mengarelli A
- Menke S
- Meoni E
- Mergelmeyer S
- Merino JL
- Mermod P
- Merola L
- Meroni C
- Merritt FS
- Messina A
- Metcalfe J
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- Miguens JM
- Mijovic L
- Mikenberg G
- Mikestikova M
- Mikuz M
- Milesi M
- Milic A
- Miller DW
- Mills C
- Milosavljevic MV
- Milov A
- Milstead DA
- Minaenko AA
- Minami Y
- Minashvili IA
- Mincer AI
- Mindur B
- Mineev M
- Ming Y
- Miotto GL
- Mir LM
- Mistry KP
- Mitani T
- Mitrevski J
- Mitsou VA
- Miucci A
- Miyagawa PS
- Mjornmark JU
- Moa T
- Mochizuki K
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- Mohapatra S
- Molander S
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- Monden R
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- Monk J
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- Mori D
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- Morisbak V
- Moritz S
- Morley AK
- Mornacchi G
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- Mortensen SS
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- Mosidze M
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- Mountricha E
- Mouraviev SV
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- Muanza S
- Mudd RD
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- Muino PC
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- Muskinja M
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- Namasivayam H
- Narayan R
- Naryshkin I
- Naumann T
- Navarro G
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- Nechaeva PY
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- Nef PD
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- Nikiforov A
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- Nikolic-Audit I
- Nikolopoulos K
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- Ninomiya Y
- Nisati A
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- Novgorodova O
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- Nozka L
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- Nurse E
- Nuti F
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- Okumura Y
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- Olariu A
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- Onofre A
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- Ortiz NGG
- Ortuzar MC
- Osculati B
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- Ouchrif M
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- Padilla Aranda C
- Pagacova M
- Paige F
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- Papageorgiou K
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- Parzefall U
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- Pasqualucci E
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- Petersen BA
- Petersen TC
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- Petrolo E
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- Plotnikova E
- Plucinski P
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- Poley A
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- Polifka R
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- Popeneciu GA
- Popovic DS
- Poppleton A
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- Potamianos K
- Potrap IN
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- Potter CT
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- Poveda J
- Pozdnyakov V
- Pralavorio P
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- Prokoshin F
- Protopopescu S
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- Quayle WB
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- Quijada JAM
- Quilty D
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- Radeka V
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- Radhakrishnan SK
- Radloff P
- Rados P
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- Ratti MG
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- Ravenscroft T
- Ravinovich I
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- Read AL
- Readioff NP
- Reale M
- Rebuzzi DM
- Redelbach A
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- Rimoldi A
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- Ristic B
- Ritsch E
- Riu I
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- Rizvi E
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- Robinson D
- Robinson JEM
- Robson A
- Roda C
- Rodina Y
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- Rodriguez LP
- Roe S
- Rogan CS
- Rohne O
- Romaniouk A
- Romano M
- Romero Adam E
- Rompotis N
- Ronzani M
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- Rosien N-A
- Rossetti V
- Rossi E
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- Rosten JHN
- Rosten R
- Rotaru M
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- Royon CR
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- Rozen Y
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- Rudolph MS
- Ruehr F
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- Rurikova Z
- Rusakovich NA
- Ruschke A
- Russell HL
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- Ruthmann N
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- Ryu S
- Ryzhov A
- Rzehorz GF
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- Saavedra AF
- Sabato G
- Sacerdoti S
- Sadrozinski HF-W
- Sadykov R
- Saez SMR
- Saha P
- Sahinsoy M
- Saimpert M
- Saito T
- Sakamoto H
- Sakurai Y
- Salamanna G
- Salamon A
- Salazar Loyola JE
- Salek D
- Salihagic D
- Salnikov A
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- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
- Sammel D
- Sampsonidis D
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- Sanchez A
- Sanchez CAS
- Sanchez FJM
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- Sander HG
- Sandhoff M
- Sandoval C
- Sandstroem R
- Sankey DPC
- Sannino M
- Sansoni A
- Santoni C
- Santonico R
- Santos H
- Santurio EV
- Sapp K
- Sapronov A
- Saraiva JG
- Sarrazin B
- Sasaki O
- Sasaki Y
- Sato K
- Sauvage G
- Sauvan E
- Savage G
- Savard P
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- Saxon J
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- Scannicchio DA
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- Schaarschmidt J
- Schacht P
- Schachtner BM
- Schaefer D
- Schaefer R
- Schaefer U
- Schaeffer J
- Schaepe S
- Schaetzel S
- Schaffer AC
- Schaile D
- Schamberger RD
- Scharf V
- Schegelsky VA
- Scheirich D
- Schernau M
- Schiavi C
- Schier S
- Schillo C
- Schioppa M
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schneider B
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock BD
- Schopf E
- Schott M
- Schovancova J
- Schramm S
- Schreyer M
- Schroeder TV
- Schuh N
- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwegler P
- Schweiger H
- Schwemling P
- Schwienhorst R
- Schwindling J
- Schwindt T
- Sciolla G
- Scuri F
- Scutti F
- Seabra LFO
- Searcy J
- Seema P
- Seidel SC
- Seiden A
- Seifert F
- Seixas JM
- Sekhniaidze G
- Sekhon K
- Sekula SJ
- Seliverstov DM
- Semprini-Cesari N
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shaikh NW
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Shatalov PB
- Shaw K
- Shaw SM
- Shcherbakova A
- Shehu CY
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shiyakova M
- Shmeleva A
- Shmeleva A
- Shochet MJ
- Shojaii S
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
- Sickles AM
- Sidebo PE
- Sidiropoulou O
- Sidorov D
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silverstein SB
- Simak V
- Simard O
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- Simion S
- Simioni E
- Simmons B
- Simon D
- Simon M
- Sinervo P
- Sinev NB
- Sioli M
- Siragusa G
- Sivoklokov SY
- Sjolin J
- Sjursen TB
- 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
- Smirnova O
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Sokhrannyi G
- Sola JDB
- Solar M
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Song HY
- Sood A
- Sopczak A
- Sopko V
- Sorin V
- Sosa D
- Sotiropoulou CL
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spettel F
- Spighi R
- Spigo G
- Spiller LA
- Spousta M
- St Denis RD
- St Panagiotopoulou E
- Stabile A
- Stamen R
- Stamm S
- Stanecka E
- Stanek RW
- Stanescu C
- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark GH
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- Staroba P
- Starovoitov P
- Starz S
- Staszewski R
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stewart GA
- Stillings JA
- Stockton MC
- Stoebe M
- Stoicea G
- Stolte P
- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strandlie A
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Subramaniam R
- Suchek S
- Sugaya Y
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
- Taccini C
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Taiblum N
- Takai H
- Takashima R
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tan KG
- Tanaka J
- Tanaka R
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- Tannenwald BB
- Tapia Araya S
- Tapprogge S
- Tarem S
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tayalati Y
- Taylor AC
- Taylor GN
- Taylor PTE
- Taylor W
- Tehrani FS
- Teischinger FA
- Teixeira-Dias P
- Temming KK
- Temple D
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Theveneaux-Pelzer T
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson EN
- Thompson PD
- Thomsen LA
- Thomson E
- Thomson M
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
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- Todorov T
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- Torrence E
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- Toth J
- Touchard F
- Tovey DR
- Trefzger T
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Trischuk W
- 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
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turgeman D
- Turra R
- Turvey AJ
- Tuts PM
- Tyndel M
- Ucchielli G
- Ueda I
- Ueno R
- 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
- Usanova A
- Vacavant L
- Vacek V
- Vachon B
- Valderanis C
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallecorsa S
- Valls Ferrer JA
- Van den Wollenberg W
- Van der Deijl PC
- van der Geer R
- van der Graaf H
- van Eldik N
- van Gemmeren P
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vanguri R
- Vaniachine A
- Vankov P
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasquez JG
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloce LM
- Veloso F
- 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
- Vigne R
- 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
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Walls FMG
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- Wang C
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- Wang J
- Wang J
- Wang K
- Wang R
- Wang SM
- Wang T
- Wang T
- Wang W
- Wang X
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Washbrook A
- Watkins PM
- Watson AT
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Webb S
- Weber MS
- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weiser C
- Weits H
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner MD
- Werner P
- Wessels M
- Wetter J
- Whalen K
- Whallon NL
- Wharton AM
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- White R
- Whiteson D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- 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
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- 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
- Yakabe R
- 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
- Yen AL
- 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
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- 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
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2016
- Field of study
A search for Higgs-boson pair production in the bb ¯ bb ¯ final state is carried out with 3.2 fb −1 of proton-proton collision data collected at s √ =13 TeV with the ATLAS detector. The data are consistent with the estimated background and are used to set upper limits on the production cross section of Higgs-boson pairs times branching ratio to bb ¯ bb ¯ for both nonresonant and resonant production. In the case of resonant production of Kaluza-Klein gravitons within the Randall-Sundrum model, upper limits in the 24 to 91 fb range are obtained for masses between 600 and 3000 GeV, at the 95% confidence level. The production cross section times branching ratio for nonresonant Higgs-boson pairs is also constrained to be less than 1.22 pb, at the 95% confidence level
A922 Sequential measurement of 1 hour creatinine clearance (1-CRCL) in critically ill patients at risk of acute kidney injury (AKI)
- Author
- Abbott TE
- Abdallah RI
- Abdel-Aal IR
- Abdelmonem SA
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- Kezyte G
- Khadjibaev A
- Khaliq W
- Khine H
- Kim DJ
- Kim HJ
- Kim JM
- Kim JM
- Kim JW
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- Kim MH
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- Kim W
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- Kleinpell R
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- Knight LD
- Ko JI
- Ko SB
- Kobayashi A
- Koco E
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- Kodate A
- Kodate A
- Kokkini S
- Kolnikova I
- Komuro T
- Kondili E
- Kongpolprom N
- Kooner G
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- Kosuk ME
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- Kox M
- Kraegpoeth A
- Krenn CG
- Krishna B
- Kristof J
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- Kruger A
- Krüger A
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- Ku NS
- Kubik M
- Kubota K
- Kuebler WM
- Kulaga EV
- Kulkarni AP
- Kumari BK
- Kumbamu A
- Kunze-Szikszay N
- Kurmukov IA
- Kurth T
- Kurtz P
- Kurtz P
- Kwon HM
- Kwon HM
- Kwon WY
- Kwon WY
- Kwon WY
- Kye YC
- Kyle UG
- Kyle UG
- Labaune MA
- Labra C
- Lacerda P
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- Lafaurie M
- Lafuente E
- Lagonidis D
- Lagos R
- Lahmer T
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- Lapteva K
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- Latini R
- Latini R
- Latorre J
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- Leitao AL
- Leite RT
- Leonard H
- Leone M
- Leone M
- Lerma FA
- Lesmes SP
- Lesmes SP
- Lesmes SP
- Lesmes SP
- Lesmes SP
- Lesmes SP
- Letizia T
- Levrat Q
- Levy B
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- León JP
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- Lheureux O
- Lheureux O
- Lheureux O
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- Li SH
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- Lichtenstein D
- Lim TH
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- Lin KC
- Lin KC
- Lin KC
- Lin KC
- Lin KL
- Lin PH
- Lin SC
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- Lin WC
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- Lischinsky A
- Lissonde F
- Lissonde F
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- Liu CP
- Liu CP
- Liu CP
- Liu CP
- Liu D
- Llaurado-Serra M
- Llorente B
- Llorente MÁ
- Lobato MS
- Lobo-Civico A
- Loizou C
- Lombardo MD
- Londoño JG
- Longani N
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- Lopez GD
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- Lopez-Caler C
- Lopez-Gude MJ
- Lorini L
- Lortat-Jacob B
- Lortat-Jacob B
- Lotay R
- Loudet CI
- Louf-Durier A
- Louf-Durier A
- Louis B
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- Lozano JA
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- Lucinio NM
- Luini M
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- Lukaszewicz AC
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- MacKay A
- MacKay A
- Mackey G
- Mackey G
- MacPhee I
- Macrì M
- Madueño VP
- Maekawa K
- Maekawa K
- Maekawa K
- Maekawa K
- Maertens B
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- Maghsoudi B
- Magnanimi E
- Magnoni S
- Magret M
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- Maistry N
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- Makiko S
- Malagurski B
- Malek F
- Malo LR
- Maly M
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- Mancebo J
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- Mancino A
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- Marcos-Zambrano LJ
- Mariani M
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- Marin-Mateos H
- Marine-Vidal J
- Mariotte E
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- Martínez F
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- Martínez-Carmona JF
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- Mejías CR
- Mellis C
- Melnyk L
- Melo N
- Mendes A
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- Mendonca AV
- Mendsaikhan N
- Menendez R
- Mengelle C
- Mercat A
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- Mergulhão PJ
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- Messenger D
- Mezidi M
- Mezidi M
- Michel L
- Midwinter MJ
- Mignot T
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- Mihara Y
- Millar M
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- Mimoz O
- Min A
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- Miranda F
- Miranda R
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- Mistry M
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- Mitchell S
- Mizobuchi S
- Mizugaki A
- Mizugaki A
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- Motos A
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- Olaechea P
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- Rodríguez FG
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- Romero I
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- Salgado DR
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- Sandiumenge A
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- Savvidou S
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- Snelson C
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- Soeffker G
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- Spadaro S
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- Spahn DR
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- Spijkstra JJ
- Spronk PE
- Spronk PE
- Sprung CL
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- Stamm J
- Stamouli M
- Stanić R
- Starczewska M
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- Stiphout C
- Stocchetti N
- Stocchetti N
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- Stretti F
- Struijs A
- Stubbs C
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- Stümpfle R
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- Su PL
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- Suchomel P
- Suh GJ
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- Suh JW
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- Sun WZ
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- Suzuki T
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- Sylla P
- Sáez VC
- Sánchez B
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- Sánchez EC
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- Tabatabaei HR
- Tabei SH
- Taccone F
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- Taccone FS
- Taccone FS
- Taccone FS
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- Taggu A
- Takahashi H
- Takaki S
- Takaki S
- Takeda M
- Takeda M
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- Takei T
- Talan L
- Tamura T
- Tanaka H
- Tanaka S
- Tanaka S
- Tane N
- Tang KB
- Tang LK
- Tapia A
- Tapponnier R
- Tapponnier R
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- Tarabrin P
- Tavazzi G
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- Telli S
- Temprano-Gómez I
- Tena SA
- Tencé N
- Terzi N
- Terzi N
- Terzi N
- Terzi N
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- Thabut G
- Theodorakopoulou M
- Thies P
- Thilakasiri MC
- Thomas B
- Thompson E
- Thévenin D
- Tiainen M
- Timsit JF
- Tirkkonen J
- Tirumala S
- Tjepkema-Cloostermans MC
- Tobar M
- Tofiño AL
- Toh CH
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- Tonelotto BF
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- Topcu L
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- Winder-Rhodes S
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- Yılmaz G
- Yilmazer F
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- Yoshitake E
- You KM
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- Zepeda EM
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- Zwaag J
- Zýková I
- Álvarez JT
- Álvarez-Lerma F
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Meeting abstrac
Measurements of the top quark branching ratios into channels with leptons and quarks with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
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- Wyatt TR
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- Xella S
- Xu D
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- Yacoob S
- Yakabe R
- Yamada M
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
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- Yao W-M
- Yasu Y
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- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
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- Youssef S
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- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
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- Zalieckas J
- Zaman A
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- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
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- Zhang J
- Zhang L
- Zhang R
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- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- 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
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF Helmholtz Association, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; RGC, Hong Kong SAR, China; ISF, MINERVA, GIF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW and NCN, Poland; GRICES and FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN and the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA) and in the Tier-2 facilities worldwide
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