147 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Pan-cancer analysis of whole genomes
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- The ICGC/TCGA Pan-Cancer Analysis of Whole Genomes Consortium View Correspondence (jump link)
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- Publication venue
- Publication date
- 11/12/2019
- Field of study
Cancer is driven by genetic change, and the advent of massively parallel sequencing has enabled systematic documentation of this variation at the whole-genome scale(1-3). Here we report the integrative analysis of 2,658 whole-cancer genomes and their matching normal tissues across 38 tumour types from the Pan-Cancer Analysis of Whole Genomes (PCAWG) Consortium of the International Cancer Genome Consortium (ICGC) and The Cancer Genome Atlas (TCGA). We describe the generation of the PCAWG resource, facilitated by international data sharing using compute clouds. On average, cancer genomes contained 4-5 driver mutations when combining coding and non-coding genomic elements; however, in around 5% of cases no drivers were identified, suggesting that cancer driver discovery is not yet complete. Chromothripsis, in which many clustered structural variants arise in a single catastrophic event, is frequently an early event in tumour evolution; in acral melanoma, for example, these events precede most somatic point mutations and affect several cancer-associated genes simultaneously. Cancers with abnormal telomere maintenance often originate from tissues with low replicative activity and show several mechanisms of preventing telomere attrition to critical levels. Common and rare germline variants affect patterns of somatic mutation, including point mutations, structural variants and somatic retrotransposition. A collection of papers from the PCAWG Consortium describes non-coding mutations that drive cancer beyond those in the TERT promoter(4); identifies new signatures of mutational processes that cause base substitutions, small insertions and deletions and structural variation(5,6); analyses timings and patterns of tumour evolution(7); describes the diverse transcriptional consequences of somatic mutation on splicing, expression levels, fusion genes and promoter activity(8,9); and evaluates a range of more-specialized features of cancer genomes(8,10-18).Peer reviewe
Measurement of the cross section for inclusive isolated-photon production in pp collisions at √s=13TeV using the ATLAS detector
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- Worm SD
- Wosiek BK
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- Yamaguchi Y
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- Yao W-M
- Yap YC
- Yasu Y
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- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- 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 3.2fb−1. 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
Search for dark matter at √s=13 TeV in final states containing an energetic photon and large missing transverse momentum 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
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
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- Kataoka Y
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- Komar AA
- Komori Y
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- Kotwal A
- Koulouris A
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- Zhemchugov A
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- Zimmermann C
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- Zinser M
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- 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 fb−1 of proton–proton 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 750–1200 GeV for dark-matter candidate masses below 230–480 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 M∗ 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 Zγ and the Z boson subsequently decays into neutrinos
Measurements of integrated and differential cross sections for isolated photon pair production in pp collisions at √s=8 TeV with the ATLAS detector
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- Yildirim E
- Yildiz HD
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- Zalieckas J
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- Zemla A
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- Zhao Z
- Zhemchugov A
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- Zhou M
- Zhou N
- Zhu CG
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- 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
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of √s=8 TeV is presented. The results are based on an integrated luminosity of 20.2 fb−1 recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying |ηγ|40GeV and EγT,2>30 GeV for the two leading photons ordered in transverse energy produced in the interaction. The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is 16.8 ± 0.8 pb . The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Alberich LC
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
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- Alshehri AA
- Alstaty MI
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
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- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
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- Asimakopoulou EM
- Asquith L
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- Astigarraga MEP
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- Augsten K
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- Avramidou R
- Ayoub MK
- Azoulay AM
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- Baca MJ
- Bachacou H
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- Bailey AJ
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- Biglietti M
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- Bocchetta SS
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- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
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- Boldyrev AS
- Bolz AE
- Bomben M
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- Bonilla JS
- Boonekamp M
- Borecka-Bielska HM
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
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- Boscherini D
- Bosman M
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- Zakharchuk N
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- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zgubic M
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- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu CG
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Properties of jet fragmentation using charged particles measured with the ATLAS detector in pp collisions at root s=13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
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- Adamczyk L
- Adelman J
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- Aleksa M
- Aleksandrov IN
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/09/2019
- Field of study
This paper presents a measurement of quantities related to the formation of jets from high-energy quarks and gluons (fragmentation). Jets with transverse momentum 100 GeV 500 MeV and |η| < 2.5 are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the two leading jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons with parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark and gluon extractions using input from simulation. The simulations provide a reasonable description of the quark-like data across the jet
Pt range presented in -this measurement, but the gluon-like data have systematically fewer charged particles than the simulation
Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb−1 of s√ = 13 TeV pp collision data with the ATLAS detector
- Author
- Aaboud M
- Aad G
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- Abdinov O
- Abeloos B
- Abhayasinghe DK
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- Merola L
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- Messina A
- Metcalfe J
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- Mijovic L
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- Milic A
- Millar DA
- Miller DW
- Milosavljevic MV
- Milov A
- Milstead DA
- Minaenko AA
- Minashvili IA
- Mincer AI
- Mindur B
- Mineev M
- Minegishi Y
- Ming Y
- Miotto GL
- Mir LM
- Mirto A
- Mistry KP
- Mitani T
- Mitrevski J
- Mitsou VA
- Miucci A
- Miyagawa PS
- Mizukami A
- Mjoernmark JU
- Mkrtchyan T
- Mlynarikova M
- Moa T
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- Moreno D
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- Morgenstern M
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- Mori D
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- Morinaga M
- Morisbak V
- Morley AK
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- Morris AP
- Morris JD
- Morvaj L
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- Mosidze M
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- Mountricha E
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- Murrone A
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- Mwewa C
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- Myska M
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- Nakano I
- Nanjo H
- Napolitano F
- Narayan R
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- Naumann T
- Navarro G
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- Nayyar R
- Neal HA
- Nechaeva PY
- Nedden MZ
- Neep TJ
- Negri A
- Negrini M
- Nektarijevic S
- Nellist C
- Nelson ME
- Nemecek S
- Nemethy P
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- Neubauer MS
- Neumann M
- Newman PR
- Ng TY
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- Nibigira E
- Nickerson RB
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- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsson P
- Ninomiya Y
- Nisati A
- Nishu N
- Nisius R
- Nitsche I
- Nitta T
- Nobe T
- Noguchi Y
- Nomachi M
- Nomidis I
- Nomura MA
- Nooney T
- Nordberg M
- Norjoharuddeen N
- Novak T
- Novgorodova O
- Novotny R
- Nozka L
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- Nurse E
- Nuti F
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- O'Neil DC
- O'Rourke AA
- O'Shea V
- Oakham FG
- Oberlack H
- Obermann T
- Ocariz J
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- Oda S
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- Oide H
- Ojeda ML
- Okawa H
- Okazaki Y
- Okumura Y
- Okuyama T
- Olariu A
- Oliveira MVS
- Oliver JL
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- Olszewski A
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- Onofre A
- Onogi K
- Onyisi PUE
- Oppen H
- Oreglia MJ
- Oren Y
- Orestano D
- Orgill EC
- Orlando N
- Orr RS
- Osculati B
- Ospanov R
- Otero y Garzon G
- Otono H
- Ouchrif M
- Ould-Saada F
- Ouraou A
- Outschoorn VIM
- Ouyang Q
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- Paganini M
- Pages AP
- Palacino G
- Palazzo S
- Palestini S
- Palka M
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- Panagoulias I
- Pandini CE
- Pani P
- Panizzo G
- Paolozzi L
- Papadopoulou TD
- Papageorgiou K
- Paramonov A
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- Parzefall U
- Pascuzzi VR
- Pasner JMP
- Pasqualucci E
- Passaggio S
- Pastor ET
- Pastore F
- Pasuwan P
- Pataraia S
- Pater JR
- Pathak A
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- Paz IL
- Pearson B
- Pedersen M
- Pedro R
- Peixoto APP
- Peleganchuk SV
- Penc O
- Peng C
- Peng H
- Peralva BS
- Perego MM
- Pereira RMFR
- Perepelitsa DV
- Perez AR
- Perez MV
- Peri F
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- Perrella S
- Peshekhonov VD
- Peters K
- Peters RFY
- Petersen BA
- Petersen TC
- Petit E
- Petridis A
- Petridou C
- Petroff P
- Petrov M
- Petrucci F
- Pettee M
- Pettersson NE
- Peyaud A
- Pezoa R
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- Piacquadio G
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- Picazio A
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- Pickles RH
- Piegaia R
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- Pineda AS
- Pinfold JL
- Pino SAO
- Pinto MVB
- Pitt M
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- Pleskot V
- Plotnikova E
- Pluth D
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pogrebnyak I
- Pohl D
- Pokharel I
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Ponce JMI
- Ponomarenko D
- Pontecorvo L
- Popeneciu GA
- Pospisil S
- Potamianos K
- Potrap IN
- Potter CJ
- Potti H
- Poulsen T
- Poveda J
- Powell TD
- Pralavorio P
- Prell S
- Price D
- Primavera M
- Prince S
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
- Puri A
- Puzo P
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- Quintero DMP
- Qureshi A
- Rados P
- Ragusa F
- Rahal G
- Raine JA
- Rajagopalan S
- Rashid T
- Raspopov S
- Ratti MG
- Rauch DM
- Rauscher F
- Rave S
- Ravina B
- Ravinovich I
- Rawling JH
- Raymond M
- Read AL
- Readioff NP
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- Rebuzzi DM
- Redelbach A
- Redlinger G
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- Reed RG
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- Reiss A
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- Resconi S
- Resseguie ED
- Rettie S
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- Rezanova OL
- Reznicek P
- Ricci E
- Richter R
- Richter S
- Richter-Was E
- Ricken O
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- Rieck P
- Riegel CJ
- Rifki O
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- Rimoldi A
- Rimoldi M
- Rinaldi L
- Ripellino G
- Ristic B
- Ritsch E
- Riu I
- Rizatdinova F
- Rizvi E
- Rizzi C
- Roberts RT
- Robertson SH
- Robinson D
- Robinson JEM
- Robson A
- Rocco E
- Roda C
- Rodina Y
- Rodriguez Bosca S
- Rodriguez Rodriguez D
- Rodriguez LP
- Roe S
- Roehrig R
- Rogan CS
- Rohne O
- Roland CPA
- Roloff J
- Romaniouk A
- Romano M
- Rompotis N
- Ronzani M
- Roos L
- Rosati S
- Rosbach K
- Rose P
- Rosien N-A
- Rossi E
- Rossi E
- Rossi LP
- Rossini L
- Rosten JHN
- Rosten R
- Rotaru M
- Rothberg J
- Rousseau D
- Roy D
- Rozanov A
- Rozas AJ
- Rozen Y
- Ruan X
- Rubbo F
- Ruehr F
- Ruettinger EM
- Ruiz-Martinez A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rutherfoord JP
- Ryabov YF
- Rybar M
- Rybkin G
- Ryu S
- Ryzhov A
- Rzehorz GF
- Saadi DS
- Sabatini P
- Sabato G
- Sacerdoti S
- Sadrozinski HF-W
- Sadykov R
- Saenz SRP
- Saha P
- Sahinsoy M
- Sahu A
- Saimpert M
- Saito M
- Saito T
- Sakamoto H
- Sakharov A
- Salamani D
- Salamanna G
- Salek D
- Salihagic D
- Salnikov A
- Salt J
- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
- Samarati J
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez CAS
- Sanchez FJM
- Sanchez J
- Sandaker H
- Sander CO
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sano Y
- Sansoni A
- Santoni C
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- Santra A
- Santurio EV
- Sapronov A
- Saraiva JG
- Sasaki O
- Sato K
- Sauvan E
- Savard P
- Savic N
- Sawada R
- Sawyer C
- Sawyer L
- Sbarra C
- Sbrizzi A
- Scanlon T
- Schaarschmidt J
- Schacht P
- Schachtner BM
- Schaefer D
- Schaefer L
- Schaefer U
- Schaeffer J
- Schaepe S
- Schaffer AC
- Schaile D
- Schamberger RD
- Scharmberg N
- Schegelsky VA
- Scheirich D
- Schenck F
- Schernau M
- Schiavi C
- Schier S
- Schildgen LK
- Schillaci ZM
- Schioppa EJ
- Schioppa M
- Schleicher KE
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schmoeckel JC
- Schnoor U
- Schoeffel L
- Schoening A
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schulte A
- Schultz-Coulon H-C
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schweiger H
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scornajenghi M
- Scuri F
- Scutti F
- Scyboz LM
- Seabra LFO
- Searcy J
- Sebastiani CD
- Seema P
- Seidel SC
- Seiden A
- Seiss T
- Seixas JM
- Sekhniaidze G
- Sekhon K
- Sekula SJ
- Semprini-Cesari N
- Sen S
- Senkin S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shahinian JD
- Shaikh NW
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Sharma A
- Sharma AS
- Shatalov PB
- Shaw K
- Shaw SM
- Shcherbakova A
- Shen Y
- Sherafati N
- Sherman AD
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet MJ
- Shojaii S
- Shope DR
- Shrestha S
- Shulga E
- Sicho P
- Sickles AM
- Sidebo PE
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silva M
- Silverstein SB
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- Simion S
- Simioni E
- Simon M
- Simoniello R
- Sinervo P
- Sinev NB
- Sioli M
- Siragusa G
- Siral I
- Sivoklokov SY
- Sjoelin J
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smith MNK
- Smizanska M
- Smolek K
- Smykiewicz A
- Snesarev AA
- Snyder IM
- Snyder S
- Sobie R
- Soffa AM
- Soffer A
- Sogaard A
- Soh DA
- Sokhrannyi G
- Solar M
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Song W
- Song WY
- Sopczak A
- Sopkova F
- Sosa D
- Sotiropoulou CL
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spettel F
- Spieker TM
- Spighi R
- Spigo G
- Spiller LA
- Spiteri DP
- Spousta M
- Stabile A
- Staerz S
- Stamen R
- Stamm S
- Stanecka E
- Stanek RW
- Stanescu C
- Stanislaus B
- Stanitzki MM
- Stapf B
- Stapnes S
- Starchenko EA
- Stark GH
- Stark J
- Stark SH
- Staroba P
- Starovoitov P
- Staszewski R
- Stegler M
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Sterzo FL
- Stevenson TJ
- Stewart GA
- Stockton MC
- Stoicea G
- Stolte P
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
- Su J
- Suchek S
- Sugaya Y
- Suk M
- Sulin VV
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Sydorenko A
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Tahirovic E
- Taiblum N
- Takai H
- Takashima R
- Takasugi EH
- Takeda K
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tanaka J
- Tanaka M
- Tanaka R
- Tannenwald BB
- Tapprogge S
- Tarem S
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tayalati Y
- Taylor AC
- Taylor AJ
- Taylor GN
- Taylor PTE
- Taylor W
- Tee AS
- Tehrani FS
- Teixeira-Dias P
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Thais SJ
- Theenhausen HMZ
- Theveneaux-Pelzer T
- Thiele F
- Thomas DW
- Thomas JP
- Thompson AS
- Thompson PD
- Thomsen LA
- Thomson E
- Tian Y
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Tobon CAM
- Todome K
- Todorova-Nova S
- Todt S
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
- Tomiwa KG
- Tomoto M
- Tompkins L
- Toms K
- Tong B
- Tornambe P
- Toro RC
- Torrence E
- Torres H
- Torres RET
- Tosciri C
- Toth J
- Touchard F
- Tovey DR
- Treado CJ
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trovatelli M
- Trovato F
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tseng JC-L
- Tsiareshka PV
- Tsirigotis A
- Tsirintanis N
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
- Turra R
- Tuts PM
- Tzovara E
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Urban J
- Urquijo P
- Urrejola P
- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Valls Ferrer JA
- Van Daalen TR
- Van der Graaf H
- Van Gemmeren P
- Van Nieuwkoop J
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Vazquez JGP
- Veatch J
- Vecchio V
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Vera AMR
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Verzini MJA
- Vetterli MC
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Villa M
- Villar DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vogel M
- Vokac P
- Volpi G
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Wakamiya K
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang C
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang P
- Wang Q
- Wang R
- Wang R
- Wang R-J
- Wang SM
- Wang W
- Wang WT
- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Washbrook A
- Watkins PM
- Watson AT
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Webb AF
- Webb S
- Weber C
- Weber MS
- Weber SA
- Weber SM
- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Werner P
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Wilkins LJ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yue X
- Yuen SPY
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang D
- Zhang DF
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 17/02/2021
- Field of study
A search for the supersymmetric partners of quarks and gluons (squarks and gluinos) in final states containing jets and missing transverse momentum, but no electrons or muons, is presented. The data used in this search were recorded by the ATLAS experiment in proton-proton collisions at a centre-of-mass energy of s√ = 13 TeV during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. The results are interpreted in the context of various R-parity-conserving models where squarks and gluinos are produced in pairs or in association and a neutralino is the lightest supersymmetric particle. An exclusion limit at the 95% confidence level on the mass of the gluino is set at 2.30 TeV for a simplified model containing only a gluino and the lightest neutralino, assuming the latter is massless. For a simplified model involving the strong production of mass-degenerate first- and second-generation squarks, squark masses below 1.85 TeV are excluded if the lightest neutralino is massless. These limits extend substantially beyond the region of supersymmetric parameter space excluded previously by similar searches with the ATLAS detector
Search for heavy diboson resonances in semileptonic final states in pp collisions at s√=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 17/12/2020
- Field of study
This paper reports on a search for heavy resonances decaying into WW, ZZ or WZ using proton–proton collision data at a centre-of-mass energy of s√=13 TeV. The data, corresponding to an integrated luminosity of 139 fb1, were recorded with the ATLAS detector from 2015 to 2018 at the Large Hadron Collider. The search is performed for final states in which one W or Z boson decays leptonically, and the other W boson or Z boson decays hadronically. The data are found to be described well by expected backgrounds. Upper bounds on the production cross sections of heavy scalar, vector or tensor resonances are derived in the mass range 300–5000 GeV within the context of Standard Model extensions with warped extra dimensions or including a heavy vector triplet. Production through gluon–gluon fusion, Drell–Yan or vector-boson fusion are considered, depending on the assumed model
Search for doubly and singly charged Higgs bosons decaying into vector bosons in multi-lepton final states with the ATLAS detector using proton-proton collisions at s√ = 13 TeV
- Author
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- Aad G
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- Abdinov O
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- Zemaityte G
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- Zhemchugov A
- Zhou B
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- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
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- Zobernig G
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- Zorbas TG
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- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 24/06/2021
- Field of study
A search for charged Higgs bosons decaying into W±W± or W±Z bosons is performed, involving experimental signatures with two leptons of the same charge, or three or four leptons with a variety of charge combinations, missing transverse momentum and jets. A data sample of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded with the ATLAS detector at the Large Hadron Collider between 2015 and 2018 is used. The data correspond to a total integrated luminosity of 139 fb−1. The search is guided by a type-II seesaw model that extends the scalar sector of the Standard Model with a scalar triplet, leading to a phenomenology that includes doubly and singly charged Higgs bosons. Two scenarios are explored, corresponding to the pair production of doubly charged H±± bosons, or the associated production of a doubly charged H±± boson and a singly charged H± boson. No significant deviations from the Standard Model predictions are observed. H±± bosons are excluded at 95% confidence level up to 350 GeV and 230 GeV for the pair and associated production modes, respectively
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