146 research outputs found
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aesky S
- Agar-Savedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
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- Allison LJ
- Allport PP
- Allwood-Spiers SE
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- Arguin J-F
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- Armbruster AJ
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- Artamonov A
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- Arutinov D
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or Ï lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, Ï, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan ÎČ in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
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
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- Zanzi D
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- Zhemchugov A
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- 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 4.5ââfb[superscript â1] of proton-proton collisions data at âs=7ââTeV and 20.3ââfb[superscript â1] at âs=8ââTeV 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 ÎŒ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4ââGeV. 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 ÎŒ[subscript ggF]=1.32±0.38, ÎŒ[subscript VBF]=0.8±0.7, ÎŒ[subscript WH]=1.0±1.6, ÎŒ[subscript ZH]=0.1[superscript +3.7 subscript â0.1], and ÎŒ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript â1.8], 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 differential cross sections and W + /W â cross-section ratios for W boson production in association with jets at âs =8 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Alberich L Cerda
- Albert J
- Albicocco P
- Alderweireldt SC
- 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
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- Alshehri AA
- Alstaty MI
- Alviggi MG
- Amadio BT
- Amelung C
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- Anastopoulos C
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- Anderson KJ
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- Angelidakis S
- Angelozzi I
- Angerami A
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- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
This paper presents a measurement of the W boson production cross section and the W + /W â cross-section ratio, both in association with jets, in proton--proton collisions at s â =8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb â1 . Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W + /W â the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proto
Measurements of normalized differential cross sections for ttÌ production in pp collisions at â(s)=7ââTeV using the ATLAS detector
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- Yildiz HD
- Yilmaz M
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- Yoshihara K
- Young C
- Young CJS
- Youssef S
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- Yu J
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- Yu JM
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
Measurements of normalized differential cross sections for top-quark pair production are presented as a function of the top-quark transverse momentum, and of the mass, transverse momentum, and rapidity of the tÂŻt system, in protonâproton collisions at a center-of-mass energy of âs=7ââTeV. The data set corresponds to an integrated luminosity of 4.6ââfbâ1, recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one lepton and at least four jets with at least one of the jets tagged as originating from a b-quark. The measured spectra are corrected for detector efficiency and resolution effects and are compared to several Monte Carlo simulations and theory calculations. The results are in fair agreement with the predictions in a wide kinematic range. Nevertheless, data distributions are softer than predicted for higher values of the mass of the tÂŻt system and of the top-quark transverse momentum. The measurements can also discriminate among different sets of parton distribution functions
Measurement of the cross section for inclusive isolated-photon production in pp collisions at âs=13TeV using the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
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- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- 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
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Inclusive isolated-photon production in pp collisions at a centre-of-mass energy of 13TeVis studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2fbâ1. The cross section is measured as a function of the photon transverse energy above 125GeVin different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data
Performance of missing transverse momentum reconstruction with the ATLAS detector using protonâproton collisions at âs = 13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Abramowicz H
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- Acharya BS
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in protonâproton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying Ï -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fbâ1
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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- Zoccoli A
- zur Nedden M
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
This is an Open Access article distributed in accordance with the terms of the Creative Commons Attribution (CC BY 4.0) license, which permits others to distribute, remix, adapt and build upon this work, for commercial use, provided the original work is properly cited. See: http://creativecommons.org/ licenses/by/4.0
Modelling Z â ÏÏ processes in ATLAS with Ï-embedded Z â ΌΌ data
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- 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
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi G
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
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- Andeen T
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- Anger P
- Angerami A
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- Anisenkov AV
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- Annovi A
- Antonelli M
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- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arika M
- Armadans RC
- Armbruster AJ
- Arnaez O
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- Arnold H
- Arratia M
- Arslan O
- Artamonov A
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- Banerjee S
- Bannoura AAE
- Bansil HS
- Barajas CAC
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- Barberio EL
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- Bawa HS
- Beacham JB
- Beattie MD
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- Zalieckas J
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- Zemla A
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- Zenin O
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- Zhemchugov A
- Zhong J
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- 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
- 'IOP Publishing'
- Publication date
- 01/01/2015
- Field of study
This paper describes the concept, technical realisation and validation of a largely data-driven method to model events with ZâÏÏ decays. In ZâΌΌ events selected from proton-proton collision data recorded at âs=8 TeV with the ATLAS experiment at the LHC in 2012, the Z decay muons are replaced by Ï leptons from simulated ZâÏÏ decays at the level of reconstructed tracks and calorimeter cells. The Ï lepton kinematics are derived from the kinematics of the original muons. Thus, only the well-understood decays of the Z boson and Ï leptons as well as the detector response to the Ï decay products are obtained from simulation. All other aspects of the event, such as the Z boson and jet kinematics as well as effects from multiple interactions, are given by the actual data. This so-called Ï-embedding method is particularly relevant for Higgs boson searches and analyses in ÏÏ final states, where ZarrowÏÏ decays constitute a large irreducible background that cannot be obtained directly from data control samples. In this paper, the relevant concepts are discussed based on the implementation used in the ATLAS Standard Model HâÏÏ analysis of the full datataset recorded during 2011 and 2012
Measurements of the top quark branching ratios into channels with leptons and quarks with the ATLAS detector
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- 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 MIZĆ , 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
Searches for Higgs boson pair production in the hhâbbÏÏ, γγWWâ, γγbb, bbbb channels with the ATLAS detector
- Author
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- 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
- Mjoernmark JU
- Moa T
- Mochizuki K
- Moenig K
- Mohapatra S
- Mohr W
- Molander S
- Moles-Valls R
- Monden R
- Monini C
- Monk J
- Monnier E
- Montalbano A
- Monticelli F
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- Morange N
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- Mori T
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- Morisbak V
- Moritz S
- Morley AK
- Mornacchi G
- Morris JD
- Mortensen SS
- Morton A
- Morvaj L
- Mosidze M
- Moss J
- Motohashi K
- Mount R
- Mountricha E
- Mouraviev SV
- Moyse EJW
- Muanza S
- Mudd RD
- Mueller F
- Mueller J
- Mueller RSP
- Mueller T
- Muenstermann D
- Muino PC
- Mullen P
- Mullier GA
- Murillo Quijada JA
- Murray WJ
- Musheghyan H
- Musto E
- Myagkov AG
- Myska M
- Nachman BP
- Nackenhorst O
- Nadal J
- Nagai K
- Nagai R
- Nagai Y
- Nagano K
- Nagarkar A
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- Nagata K
- Nagel M
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- Nakahama Y
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- Nakano I
- Namasivayam H
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- Nechaeva PY
- Nedden MZ
- Neep TJ
- Nef PD
- Negri A
- Negrini M
- Nektarijevic S
- Nellist C
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- Nemecek S
- Nemethy P
- Nepomuceno AA
- Nessi M
- Neubauer MS
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- Neves RM
- Nevski P
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- Nguyen DH
- Nickerson RB
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- Nicquevert B
- Nielsen J
- Nikiforou N
- Nikiforov A
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
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- Ninomiya Y
- Nisati A
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- Nomachi M
- Nomidis I
- Nooney T
- Norberg S
- Nordberg M
- Novgorodova O
- Nowak S
- Nozaki M
- Nozka L
- Ntekas K
- Nunnemann T
- Nurse E
- Nuti F
- O'Brien BJ
- O'grady F
- O'Neil DC
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- Ogren H
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- Ohm CC
- Ohman H
- Oide H
- Okamura W
- Okawa H
- Okumura Y
- Okuyama T
- Olariu A
- Olivares Pino SA
- Oliveira Damazio D
- Olszewski A
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- Onofre A
- Onogi K
- Onyisi PUE
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- Ortuzar MC
- Osculati B
- Ospanov R
- Otero y Garzon G
- Otono H
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- Ouraou A
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- Ouyang Q
- Ovcharova A
- Owen M
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- Papadopoulou TD
- Papageorgiou K
- Paramonov A
- Paredes BL
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- Parzefall U
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- Patel ND
- Pater JR
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- Paz IL
- Pearce J
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- Petersen BA
- Petersen TC
- Petit E
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- Petrucci F
- Pettersson NE
- Pezoa R
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- Piacquadio G
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- Picazio A
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- Pilkington AD
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- Polesello G
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- Policicchio A
- Polifka R
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- Pollard CS
- Polychronakos V
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- Pontecorvo L
- Pope BG
- Popeneciu GA
- Popovic DS
- Poppleton A
- Pospisil S
- Potamianos K
- Potrap IN
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- Pozdnyakov V
- Pralavorio P
- Pranko A
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- Price LE
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- Protopapadaki E
- Protopopescu S
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- Przybycien M
- Ptacek E
- Puddu D
- Pueschel E
- Puldon D
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- Quarrie DR
- Quayle WB
- Queitsch-Maitland M
- Quilty D
- Raddum S
- Radeka V
- Radescu V
- Radhakrishnan SK
- Radloff P
- Rados P
- Ragusa F
- Rahal G
- Rajagopalan S
- Rammensee M
- Ramos JM
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- Rauscher F
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- Ravenscroft T
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- Read AL
- Readioff NP
- Rebuzzi DM
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- Redlinger G
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- Reichert J
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- Resconi S
- Rezanova OL
- Reznicek P
- Rezvani R
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- Riegel CJ
- Rieger J
- Rifki O
- Rijssenbeek M
- Rimoldi A
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- Ristic B
- Ritsch E
- Riu I
- Rizatdinova F
- Rizvi E
- Robertson SH
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- Robinson D
- Robinson JEM
- Robson A
- Roda C
- Roe S
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- Romaniouk A
- Romano M
- Rompotis N
- Ronzani M
- Roos L
- Ros E
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- Rose P
- Rosendahl PL
- Rosenthal O
- Rossetti V
- Rossi E
- Rossi LP
- Rosten JHN
- Rosten R
- Rotaru M
- Roth I
- Rothberg J
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- Royon CR
- Rozanov A
- Rozas AJ
- Rozen Y
- Ruan X
- Rubbo F
- Rubinskiy I
- Rud VI
- Rudolph C
- Rudolph MS
- Ruehr F
- Ruiz-Martinez A
- Rurikova Z
- Rusakovich NA
- Ruschke A
- Russell HL
- Rutherfoord JP
- Ruthmann N
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- Rybar M
- Rybkin G
- Ryder NC
- Ryzhov A
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- Saavedra AF
- Sabato G
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- Saddique A
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- Sadykov R
- Saez SMR
- Saha P
- Sahinsoy M
- Saimpert M
- Saito T
- Sakamoto H
- Sakurai Y
- Salamanna G
- Salamon A
- Saleem M
- Salek D
- Salihagic D
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- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
- Sammel D
- Sampsonidis D
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- Sandaker H
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- Sandhoff M
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- Sandstroem R
- Sankey DPC
- Sannino M
- Sansoni A
- Santoni C
- Santonico R
- Santos H
- 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
- Sbarra C
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- Scanlon T
- Scannicchio DA
- Scarcella M
- Scarfone V
- Schaarschmidt J
- Schacht P
- 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
- Schillo C
- Schioppa M
- Schlenker S
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitt S
- Schneider B
- Schnellbach YJ
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock BD
- Schopf E
- Schorlemmer ALS
- Schott M
- Schouten D
- Schovancova J
- Schramm S
- Schreyer M
- Schroeder TV
- Schuh N
- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwanenberger C
- Schwartzman A
- Schwarz TA
- Schwegler P
- Schweiger H
- Schwemling P
- Schwienhorst R
- Schwindling J
- Schwindt T
- Sciacca FG
- Scifo E
- Sciolla G
- Scuri F
- Scutti F
- Searcy J
- Sedov G
- Sedykh E
- 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
- Serre T
- Sessa M
- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shamim M
- 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
- Shochet MJ
- Shojaii S
- Shrestha S
- Shulga E
- Shupe MA
- Shushkevich S
- Sicho P
- Sidebo PE
- Sidiropoulou O
- Sidorov D
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silver Y
- Silverstein SB
- Simak V
- Simard O
- Simic L
- Simion S
- Simioni E
- Simmons B
- Simon D
- Sinervo P
- Sinev NB
- Sioli M
- Siragusa G
- Sisakyan AN
- Sivoklokov SY
- Sjoelin J
- Sjursen TB
- Skinner MB
- Skottowe HP
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snidero G
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Sokhrannyi G
- Solans CA
- Solar M
- Solc J
- Soldatov EY
- Soldevila U
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Song HY
- Soni N
- Sood A
- Sopczak A
- Sopko B
- Sopko V
- Sorin V
- Sosa D
- Sosebee M
- Sotiropoulou CL
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Spearman WR
- Sperlich D
- Spettel F
- Spighi R
- Spigo G
- Spiller LA
- Spousta M
- St Denis RD
- St Panagiotopoulou E
- Stabile A
- Staerz S
- Stahlman J
- Stamen R
- Stamm S
- Stanecka E
- Stanescu C
- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Steinberg P
- Stelzer B
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- 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 E
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Subramaniam R
- Succurro A
- 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
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tam JYC
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tannenwald BB
- Tannoury N
- Tapprogge S
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tayalati Y
- Taylor FE
- 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
- Theenhausen HMZ
- Theveneaux-Pelzer T
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson RJ
- Thomsen LA
- Thomson E
- Thomson M
- Thun RP
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
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- Tomoto M
- Tompkins L
- Toms K
- Toro RC
- Torregrosa EF
- Torrence E
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- Torres RET
- Toth J
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- Tovey DR
- Trefzger T
- Tremblet L
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Trischuk W
- Trocme B
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- Truong L
- Trzebinski M
- Trzupek A
- Tsarouchas C
- Tseng JC-L
- Tsiareshka PV
- Tsionou D
- 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
- Turra R
- Turvey AJ
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Ueda I
- Ueno R
- Ughetto M
- Ugland 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
- 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
- Vandelli W
- Vanguri R
- Vaniachine A
- Vannucci F
- Vaque FV
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloce LM
- Veloso F
- Velz T
- Veneziano S
- Ventura A
- Ventura D
- 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
- Vigne R
- Villa M
- Villar DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt H
- von Radziewski 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
- Walls FMG
- Wang C
- Wang F
- Wang H
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- Wang J
- Wang J
- Wang K
- Wang R
- Wang SM
- Wang T
- Wang T
- Wang X
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Washbrook A
- Wasicki C
- Watkins PM
- Watson AT
- Watson IJ
- 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
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- Wessels M
- Wetter J
- Whalen K
- Wharton AM
- White A
- White MJ
- White R
- White S
- Whiteson D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson A
- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- 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
- Yamada M
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- 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
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- 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 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
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
Searches for both resonant and nonresonant Higgs boson pair production are performed in the hhâbbÏÏ, γγWWâ final states using 20.3ââfbâ1 of pp collision data at a center-of-mass energy of 8 TeV recorded with the ATLAS detector at the Large Hadron Collider. No evidence of their production is observed and 95% confidence-level upper limits on the production cross sections are set. These results are then combined with the published results of the hhâγγbb, bbbb analyses. An upper limit of 0.69 (0.47) pb on the nonresonant hh production is observed (expected), corresponding to 70 (48) times the SM ggâhh cross section. For production via narrow resonances, cross-section limits of hh production from a heavy Higgs boson decay are set as a function of the heavy Higgs boson mass. The observed (expected) limits range from 2.1 (1.1) pb at 260 GeV to 0.011 (0.018) pb at 1000 GeV. These results are interpreted in the context of two simplified scenarios of the Minimal Supersymmetric Standard Model
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