127 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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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
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- Zimmermann S
- Zinonos Z
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- 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
- 01/01/2015
- 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
Mechanisms of human telomerase reverse transcriptase (hTERT) regulation: clinical impacts in cancer
- Author
- A Azouz
- A Kilian
- A Kulic
- A Portela
- A Zhang
- AA Avilion
- AF Vallarelli
- AG Bodnar
- AH Shain
- AJ Bannister
- AJ Cesare
- AK Chan
- AM Deaton
- Arnaldo Figueiredo
- AS Venteicher
- B McClintock
- B Seynnaeve
- B van Steensel
- B Vogelstein
- C Cifuentes-Rojas
- C Harle-Bachor
- CB Harley
- CB Umbricht
- CB Umbricht
- CD Hurst
- CM Counter
- CM Croce
- CP Morales
- CW Greider
- D Broccoli
- D Hanahan
- DG Albertson
- DL Aisner
- DM Cittelly
- Donghyun Lee
- DS Huang
- E Naderlinger
- E Nagore
- EH Blackburn
- F Ishikawa
- F Peng
- FW Huang
- G Cimino-Reale
- G Cristofari
- G Di Leva
- G Furtjes
- GB Morin
- GC Prendergast
- H Populo
- H Suzuki
- H Tahara
- H Xie
- H Zhang
- HH Ng
- I Guilleret
- I Hatada
- I Kinde
- J Deng
- J Feng
- J Li
- J Vinagre
- J Vinagre
- J Winter
- J Zhou
- JA Weber
- JC Nault
- JD Griffith
- JE Koziel
- JG Herman
- JH Choi
- JL Stern
- Joana Dias Apolónio
- JW Catto
- JW Shay
- JW Shay
- JW Shay
- JW Shay
- K Chiba
- K Gao
- K Hiyama
- K Huppi
- K Liu
- K Vincent
- K Yoshida
- K Yoshida
- KA Hoadley
- KA Lewis
- KH Shin
- KJ Wu
- L Bai
- L Chen
- L Cheng
- L Harrington
- L Liu
- LA Carey
- LG Perez-Rivas
- LJ Valentijn
- M Esteller
- M Kawashima
- M Kochling
- M Peifer
- M Wick
- M Xing
- M Xing
- M Zimmermann
- MA Jafri
- MA Shammas
- MJ Ahn
- MK Graham
- N Wang
- N Wang
- NG Lopatina
- NJ Fredriksson
- NW Kim
- P Castelo-Branco
- P Castelo-Branco
- P Martinez
- P Ostling
- P Yuan
- Pedro Castelo-Branco
- PJ Killela
- PJ Killela
- PS Rachakonda
- PV Glybochko
- R Hrdlickova
- R Liu
- R Meier
- R Pinyol
- R Rupaimoole
- R Stoehr
- RA Breslow
- RD Ramirez
- Ricardo Leão
- RJ Bell
- RK Moyzis
- RL Zinn
- S Borah
- S Horn
- S Kyo
- S Kyo
- S Kyo
- S Mitomo
- S Piscuoglio
- S Renaud
- S Saxonov
- S Wu
- SA Bert
- SB Baylin
- SB Cohen
- SC Akincilar
- SC Mack
- SK Dessain
- SL Weinrich
- T de Lange
- T de Lange
- T Fernandez-Marcelo
- T Saito
- T Saito
- T Tsujioka
- T Vulliamy
- TE Bartlett
- TL Beattie
- TM Bryan
- TM Nakamura
- TP Brien
- TR Devereux
- Uri Tabori
- WC Cho
- WE Wright
- WE Wright
- X Liu
- X Liu
- X Xu
- X Zhao
- XJ Yi
- Y Allory
- Y Doksani
- Y Lin
- Y Wu
- YS Cong
- YS Cong
- Z Li
- ZY Zhang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2018
- Field of study
Background
Limitless self-renewal is one of the hallmarks of cancer and is attained by telomere maintenance, essentially through telomerase (hTERT) activation. Transcriptional regulation of hTERT is believed to play a major role in telomerase activation in human cancers.
Main body
The dominant interest in telomerase results from its role in cancer. The role of telomeres and telomere maintenance mechanisms is well established as a major driving force in generating chromosomal and genomic instability. Cancer cells have acquired the ability to overcome their fate of senescence via telomere length maintenance mechanisms, mainly by telomerase activation.
hTERT expression is up-regulated in tumors via multiple genetic and epigenetic mechanisms including hTERT amplifications, hTERT structural variants, hTERT promoter mutations and epigenetic modifications through hTERT promoter methylation. Genetic (hTERT promoter mutations) and epigenetic (hTERT promoter methylation and miRNAs) events were shown to have clinical implications in cancers that depend on hTERT activation. Knowing that telomeres are crucial for cellular self-renewal, the mechanisms responsible for telomere maintenance have a crucial role in cancer diseases and might be important oncological biomarkers. Thus, rather than quantifying TERT expression and its correlation with telomerase activation, the discovery and the assessment of the mechanisms responsible for TERT upregulation offers important information that may be used for diagnosis, prognosis, and treatment monitoring in oncology. Furthermore, a better understanding of these mechanisms may promote their translation into effective targeted cancer therapies.
Conclusion
Herein, we reviewed the underlying mechanisms of hTERT regulation, their role in oncogenesis, and the potential clinical applications in telomerase-dependent cancers.info:eu-repo/semantics/publishedVersio
Multi-messenger observations of a binary neutron star merger
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- Aartsen MG
- Abbott BP
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- Akras S
- Al Samarai I
- Albert A
- Albert A
- Albuquerque IFM
- Albury JM
- Alcaniz JS
- Alexander KD
- Alfaro R
- Alighieri S Di Serego
- Allam S
- Allekotte I
- Allen B
- Allen G
- Allison J
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- Alvarez C
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- Areeda JS
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- Array LWA Long Wavelength
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- Li X
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- Li XB
- Li XF
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- Pandya H
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- Pang B
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- Pannarale F
- Pant BC
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- Paoletti F
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- Parmiggiani N
- Parra A
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- Passaquieti R
- Passuello D
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- Pavalas GE
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- Pea-Rodriguez J
- Pearlstone BL
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- Pekeur NW
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- Piccinni OJ
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- Pierro V
- Pignata G
- Pike S
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- Pinto IM
- Piotrowski LW
- Piran T
- Piran T
- Piranomonte S
- Pirello M
- Piro AL
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- Piron F
- Pirronello V
- Pisanu T
- Pita S
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- Podsiadlowski P
- Poe M
- Poggiani R
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- Pollmann A Obertacke
- Poolakkil S
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- Popolizio P
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- Pozanenko AS
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- Prado RR
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- Principe G
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- Prochaska JX
- Prodi GA
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- Prokhorov LG
- Prokoph H
- Prouza M
- Prrer M
- Przybylski GT
- Pulone L
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- Quimby RM
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- Reimer A
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- Reitze DH
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- Ren Z
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- Renzi V
- Reposeur T
- Resconi E
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- Rest A
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- Reyes R De Los
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- Riccobene G
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- Riviere C
- Rizi V
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- Robie R
- Robinet F
- Rocchi A
- Rochester LS
- Rodi J
- Rodriguez H
- Rojas D Avila
- Rojas-Bravo C
- Rojo J Rodriguez
- Rol E
- Rolland L
- Rollins JG
- Roma VJ
- Romano R
- Romel CL
- Romer AK
- Romero M Dominguez
- Romie JH
- Romoli C
- Roncoroni MJ
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- Roques J-P
- Rosa-Gonzlez D
- Rosell A Carnero
- Rosenberg M
- Rosetti S
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- Ross MP
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- Rosswog S
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- Roth M
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- Rowlinson A
- Rowlinson A
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- Rudak B
- Ruehl P
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- Ruiz R Gracia
- Ruiz-Velasco E
- Rulten CB
- Rumyantsev VV
- Rusu F
- Rutins G
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- Ryckbosch D
- Rykoff ES
- Rysewyk D
- Saba A
- Sachdev S
- Sadecki T
- Sadeghian L
- Sadler EM
- Sadler EM
- Saffe C
- Saffi SJ
- Saftoiu A
- Sahakian V
- Sai N
- Saito S
- Saito T
- Saito Y
- Sakamaki A
- Sakamoto T
- Sakellariadou M
- Sako M
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- Salafia OS
- Salamida F
- Salazar H
- Salazar H
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- Saldaa M
- Saleem M
- Saleh A
- Salemi F
- Salina G
- Salmon L
- Salvadori I
- Salvaterra R
- Samajdar A
- Sammut L
- Sampedro L
- Sampson LM
- Samtleben DFE
- Sanchez B
- Sanchez DA
- Sanchez E
- Sanchez EJ
- Sanchez F
- Sanchez LE
- Sanchez-Losa A
- Sanchez-Lucas P
- Sanchez-Ramirez R
- Sanchis-Gual N
- Sand DJ
- Sandberg V
- Sanders JR
- Sandoval A
- Sandrock A
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- Santangelo A
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- Santos EM
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- Sarazin F
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- Satalecka K
- Sathyaprakash BS
- Sato R
- Saulson PR
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- Sauter O
- Savage RL
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- Sawadsky A
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- Schlegel DJ
- Schlickeiser R
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- Schmidt BP
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- Schnabel R
- Schneider A
- Schneider M
- Schneiter M
- Schoenell W
- Schoenen S
- Schofield RMS
- Scholten O
- Schonbeck A
- Schoneberg S
- Schoorlemmer H
- Schovnek P
- Schreiber E
- Schroder FG
- Schroder S
- Schroder SL
- Schssler F
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- Schuette D
- Schulte BW
- Schultz ASB
- Schulz A
- Schulz A
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- Schumacher J
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- Schwalbe SG
- Schwanke U
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- Schweyer T
- Sciutto SJ
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- Scott J
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- Secco LF
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- Segreto A
- Seidel E
- Seitenzahl IR
- Sekiguchi Y
- Sellers D
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- Sengupta AS
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- Sergeev A
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- Seunarine S
- Sevilla-Noarbe I
- Seyffert AS
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- Shah AA
- Shahriar MS
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- Shannon RM
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- Sharp RG
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- Shilon I
- Shimizu Y
- Shimomukai R
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- Shoemaker DH
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- Siemens X
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- Singer LP
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- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
Performance of the upgraded PreProcessor of the ATLAS Level-1 Calorimeter Trigger
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- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- 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 H Meyer
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2020
- Field of study
The PreProcessor of the ATLAS Level-1 Calorimeter Trigger prepares the analogue trigger signals sent from the ATLAS calorimeters by digitising, synchronising, and calibrating them to reconstruct transverse energy deposits, which are then used in further processing to identify event features. During the first long shutdown of the LHC from 2013 to 2014, the central components of the PreProcessor, the Multichip Modules, were replaced by upgraded versions that feature modern ADC and FPGA technology to ensure optimal performance in the high pile-up environment of LHC Run 2. This paper describes the features of the newMultichip Modules along with the improvements to the signal processing achieved.ANPCyTYerPhI, ArmeniaAustralian Research CouncilBMWFW, AustriaAustrian Science Fund (FWF)Azerbaijan National Academy of Sciences (ANAS)SSTC, BelarusNational Council for Scientific and Technological Development (CNPq)Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP)Natural Sciences and Engineering Research Council of CanadaCanada Foundation for InnovationNational Natural Science Foundation of China (NSFC)Departamento Administrativo de Ciencia, Tecnología e Innovación ColcienciasMinistry of Education, Youth & Sports - Czech Republic
Czech Republic GovernmentCzech Republic GovernmentDNRF, DenmarkDanish Natural Science Research CouncilCentre National de la Recherche Scientifique (CNRS)CEA-DRF/IRFU, FranceFederal Ministry of Education & Research (BMBF)Max Planck SocietyGreek Ministry of Development-GSRTRGC and Hong Kong SAR, ChinaIsrael Science FoundationBenoziyo Center, IsraelIstituto Nazionale di Fisica Nucleare (INFN)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)
Japan Society for the Promotion of ScienceCNRST, MoroccoRCN, NorwayPortuguese Foundation for Science and TechnologyMNE/IFA, RomaniaMES of RussiaMESTD, SerbiaMSSR, SlovakiaSlovenian Research Agency - SloveniaMIZS, SloveniaSpanish GovernmentSRC, SwedenWallenberg Foundation, SwedenSNSF Geneva, SwitzerlandMinistry of Science and Technology, TaiwanMinistry of Energy & Natural Resources - TurkeyScience & Technology Facilities Council (STFC)United States Department of Energy (DOE)National Science Foundation (NSF)BCKDF, CanadaCANARIE, CanadaCRC, CanadaEuropean Research Council (ERC)European Union (EU)French National Research Agency (ANR)German Research Foundation (DFG)Alexander von Humboldt FoundationGreek NSRF, GreeceBSF-NSF, IsraelGerman-Israeli Foundation for Scientific Research and DevelopmentLa Caixa Banking Foundation, SpainCERCA Programme Generalitat de Catalunya, SpainPROMETEO, SpainGenT Programmes Generalitat Valenciana, SpainGoran Gustafssons Stiftelse, SwedenRoyal Society of LondonLeverhulme TrustNRC, CanadaCERNANID, ChileChinese Academy of SciencesMinistry of Science and Technology, ChinaSRNSFG, GeorgiaHGF, GermanyNetherlands Organization for Scientific Research (NWO)
Netherlands GovernmentMinistry of Science and Higher Education, PolandNCN, PolandNRCKI, Russia FederationJINRDST/NRF, South AfricaSERI, Geneva, SwitzerlandCantons of Bern and Geneva, SwitzerlandCompute Canada, CanadaHorizon 2020Marie Sklodowska-Curie ActionsEuropean Cooperation in Science and Technology (COST)EU-ESF, Greec
Erratum: Measurement of angular and momentum distributions of charged particles within and around jets in Pb + Pb and pp collisions at √sNN = 5.02 TeV with the ATLAS detector [Phys. Rev. C 100 , 064901 (2019)]
- Author
- Aad G
- Abbott B
- Abbott Dc
- Abed Abud A
- Abeling K
- Abhayasinghe Dk
- Abidi Sh
- Abouzeid Os
- Abraham Nl
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya Bs
- Achkar B
- Adachi S
- Adam Bourdarios C
- 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
- Ahmed Ws
- Ai X
- Aielli G
- Akatsuka S
- Akesson Tpa
- Akilli E
- Akimov Av
- Al Khoury K
- Alberghi Gl
- Albert J
- Alconada Verzini Mj
- Alderweireldt S
- Aleksa M
- Aleksandrov In
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Alimonti G
- Alison J
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- Sanchez J
- Sandaker H
- Sander Co
- Sanderswood Ig
- Sandhoff M
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- Sankey Dpc
- Sannino M
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- Santoni C
- Santos H
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- Santra A
- Sapronov A
- Saraiva Jg
- Sasaki O
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- Schioppa M
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- Schmitt S
- Schmitz S
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- Schnoor U
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- Schopf E
- Schott M
- Schouwenberg Jfp
- Schovancova J
- Schramm S
- Schroeder F
- Schulte A
- Schultz-Coulon H-
- Schumacher M
- Schumm Ba
- Schune P
- Schwartzman A
- Schwarz Ta
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scodeggio M
- Scornajenghi M
- Scuri F
- Scutti F
- Scyboz Lm
- Sebastiani Cd
- Seema P
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- Seiden A
- Seidlitz Bd
- Seiss T
- Seixas Jm
- Sekhniaidze G
- Sekhon K
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- 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
- Shaked Renous D
- Shan Ly
- Shang R
- Shank Jt
- Shapiro M
- Sharma A
- Sharma As
- Shatalov Pb
- Shaw K
- Shaw Sm
- Shcherbakova A
- Shehade M
- Shen Y
- Sherafati N
- Sherman Ad
- Sherwood P
- Shi L
- Shimizu S
- Shimmin Co
- Shimogama Y
- Shimojima M
- Shipsey Ipj
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet Mj
- Shojaii J
- Shope Dr
- Shrestha S
- Shrif Em
- Shulga E
- Sicho P
- Sickles Am
- Sidebo Pe
- Sideras Haddad E
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva Oliveira Mv
- Silva Mj
- Silverstein Sb
- Simion S
- Simioni E
- Simoniello R
- Simsek S
- Sinervo P
- Sinetckii V
- Sinev Nb
- Sioli M
- Siral I
- Sivoklokov Sy
- Sjolin J
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart Bh
- Smiesko J
- Smirnov N
- Smirnov Sy
- Smirnov Y
- Smirnova Ln
- Smirnova O
- Smith Jw
- Smizanska M
- Smolek K
- Smykiewicz A
- Snesarev Aa
- Snoek Hl
- Snyder Im
- Snyder S
- Sobie R
- Soffer A
- Sogaard A
- Sohns F
- Solans Sanchez Ca
- Soldatov Ey
- Soldevila U
- Solodkov Aa
- Soloshenko A
- Solovyanov Ov
- Solovyev V
- Sommer P
- Son H
- Song W
- Song Wy
- Sopczak A
- Sopkova F
- Sotiropoulou Cl
- Sottocornola S
- Soualah R
- Soukharev Am
- South D
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spieker Tm
- Spighi R
- Spigo G
- Spina M
- Spiteri Dp
- Spousta M
- Stabile A
- Stamas Bl
- Stamen R
- Stamenkovic M
- Stanecka E
- Stanislaus B
- Stanitzki Mm
- Stankaityte M
- Stapf B
- Starchenko Ea
- Stark Gh
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- Starovoitov P
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- Staszewski R
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- Stegler M
- Steinberg P
- Steinhebel Al
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- Stockton Mc
- Stoicea G
- Stolarski M
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- Straessner A
- Strandberg J
- Strandberg S
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- Strizenec P
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- Styles Na
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- Sullivan Mj
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- Sumida T
- Sun S
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- Suruliz K
- Suster Cje
- Sutton Mr
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift Sp
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
- Sykora T
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- Taenzer J
- Taffard A
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- Takai H
- Takashima R
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- Takeshita T
- Takeva Ep
- Takubo Y
- Talby M
- Talyshev Aa
- Tamir Nm
- Tanaka J
- Tanaka M
- Tanaka R
- Tapia Araya S
- Tapprogge S
- Tarek Abouelfadl Mohamed A
- Tarem S
- Tariq K
- Tarna G
- Tartarelli Gf
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor Aj
- Taylor Gn
- Taylor W
- Tee As
- Teixeira De Lima R
- Teixeira-Dias P
- Ten Kate H
- Teoh Jj
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher Rj
- Thais Sj
- Theveneaux-Pelzer T
- Thiele F
- Thomas Dw
- Thomas Jo
- Thomas Jp
- Thompson As
- Thompson Pd
- Thomsen La
- Thomson E
- Thorpe Ej
- Ticse Torres Re
- Tikhomirov Vo
- Tikhonov Ya
- Timoshenko S
- Tipton P
- Tisserant S
- Todome K
- Todorova-Nova S
- Todt S
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
- Tomiwa Kg
- Tomoto M
- Tompkins L
- Tong B
- Tornambe P
- Torrence E
- Torres H
- Torro Pastor E
- Tosciri C
- Toth J
- Tovey Dr
- Traeet A
- Treado Cj
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger Im
- Trincaz-Duvoid S
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trovatelli M
- Trovato F
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tseng JC-
- Tsiareshka Pv
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze Eg
- Tsopoulou M
- Tsukerman Ii
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure Tt
- Tuna An
- Turchikhin S
- Turgeman D
- Turk Cakir I
- Turner Rj
- Turra Rt
- Tuts Pm
- Tzamarias S
- Tzovara E
- Ucchielli G
- Uchida K
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro Fc
- Unno Y
- Uno K
- Urban J
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- Usai G
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- Valente M
- Valentinetti S
- Valero A
- Valery L
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- Vallier A
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- Van Gemmeren P
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandewall Er
- Vaniachine A
- Vannicola D
- Vari R
- Varnes Ew
- Varni C
- Varol T
- Varouchas D
- Varvell Ke
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- Vasquez Ga
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- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Veatch J
- Vecchio V
- Veen Mj
- Veloce Lm
- Veloso F
- Veneziano S
- Ventura A
- Venturi N
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergel Infante Cm
- Vergis C
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- Vermeulen At
- Vermeulen Jc
- Vetterli Mc
- Viaux Maira N
- Vicente Barreto Pinto M
- Vickey Boeriu Oe
- Vickey T
- Viehhauser Gha
- Vigani L
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter Mg
- Virdee Gs
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
- Von Buddenbrock Se
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld Jh
- Vozak M
- Vranjes Milosavljevic M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
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- Wahdan S
- Wahlberg H
- Walbrecht Vm
- Walder J
- Walker R
- Walker Sd
- Walkowiak W
- Wallangen V
- Wang Am
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- Wang P
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- Wang W
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- Wang Wx
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward Cp
- Wardrope Dr
- Warrack N
- Washbrook A
- Watson At
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- Watts G
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- Webb Af
- Webb S
- Weber C
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- Weidberg Ar
- Weingarten J
- Weirich M
- Weiser C
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- Wengler T
- Wenig S
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- Wessels M
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- Whallon Nl
- Wharton Am
- White A
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- White Mj
- Whiteson D
- Whitmore Bw
- Wiedenmann W
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs Lam
- 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
- Wolker Rw
- Wollrath J
- Wolter Mw
- Wolters H
- Wong Vws
- Woods Nl
- Worm Sd
- Wosiek Bk
- Wozniak Kw
- Wraight K
- Wu Sl
- Wu X
- Wu Y
- Wyatt Tr
- Wynne Bm
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup Dp
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang Hj
- Yang Ht
- Yang S
- Yang X
- Yang Y
- Yao W-
- Yap Yc
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yexley Mr
- Yigitbasi E
- Yorita K
- Yoshihara K
- Young C
- Young Cjs
- Yu J
- Yuan R
- Yue X
- Yuen Spy
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev Am
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas Dr
- Zeissner Sv
- Zeitnitz C
- Zemaityte G
- Zeng Jc
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang Df
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou Ms
- Zhou N
- Zhou Y
- Zhu C
- Zhu Cg
- Zhu H
- Zhu Hl
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine Ni
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas Tg
- Zou R
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2020
- Field of study
Dijet Resonance Search with Weak Supervision Using root S=13 TeV pp Collisions in the ATLAS Detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- 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
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Banerjee S
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro F
- Barron U
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Belfkir M
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Berthold A
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
- Bhattarai P
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boutle SK
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Bullard BA
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cantero J
- Cao T
- Cao Y
- Capriles FGD
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carter JWS
- Carter TM
- Casado MP
- Casha AF
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavallaro E
- Cavasinni V
- Celebi E
- Celli F
- Cerda Alberich L
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chau CC
- Che S
- Chekanov S
- Chekulaev S
- Chelkov GA
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov M
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Chytka L
- Cieri D
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- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 25/09/2020
- Field of study
This Letter describes a search for narrowly resonant new physics using a machine-learning anomaly
detection procedure that does not rely on signal simulations for developing the analysis selection. Weakly
supervised learning is used to train classifiers directly on data to enhance potential signals. The targeted
topology is dijet events and the features used for machine learning are the masses of the two jets. The
resulting analysis is essentially a three-dimensional search A → BC, for mA ∼ OðTeVÞ, mB; mC ∼
Oð100 GeVÞ and B, C are reconstructed as large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two jets. The full run 2 ffiffi
s p ¼ 13 TeV pp collision
dataset of 139 fb−1 recorded by the ATLAS detector at the Large Hadron Collider is used for the search.
There is no significant evidence of a localized excess in the dijet invariant mass spectrum between 1.8 and
8.2 TeV. Cross-section limits for narrow-width A, B, and C particles vary with mA, mB, and mC. For
example, when mA ¼ 3 TeV and mB ≳ 200 GeV, a production cross section between 1 and 5 fb is
excluded at 95% confidence level, depending on mC. For certain masses, these limits are up to 10 times
more sensitive than those obtained by the inclusive dijet search. These results are complementary to the
dedicated searches for the case that B and C are standard model boson
Search for bottom-squark pair production in pp collision events at √s=13 TeV with hadronically decaying τ-leptons, b-jets, and missing transverse momentum using the ATLAS detector
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Zhemchugov A
- Zheng Z
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/08/2021
- Field of study
A search for pair production of bottom squarks in events with hadronically decaying
τ
-leptons,
b
-tagged jets, and large missing transverse momentum is presented. The analyzed dataset is based on proton-proton collisions at
√
s
=
13
TeV
delivered by the Large Hadron Collider and recorded by the ATLAS detector from 2015 to 2018, and corresponds to an integrated luminosity of
139
fb
−
1
. The observed data are compatible with the expected Standard Model background. Results are interpreted in a simplified model where each bottom squark is assumed to decay into the second-lightest neutralino
˜
χ
0
2
and a bottom quark, with
˜
χ
0
2
decaying into a Higgs boson and the lightest neutralino
˜
χ
0
1
. The search focuses on final states where at least one Higgs boson decays into a pair of hadronically decaying
τ
-leptons. This allows the acceptance and thus the sensitivity to be significantly improved relative to the previous results at low masses of the
˜
χ
0
2
, where bottom-squark masses up to 850 GeV are excluded at the 95% confidence level, assuming a mass difference of 130 GeV between
˜
χ
0
2
and
˜
χ
0
1
. Model-independent upper limits are also set on the cross section of processes beyond the Standard Model
Observation of electroweak production of two jets and a Z-boson pair
- Author
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- Abbott B
- Abbott DC
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- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Zenin O
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- Zgubič M
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
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- Zimmermann S
- Zinonos Z
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- Zobernig G
- Zoccoli A
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- Zwalinski L
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 09/02/2023
- Field of study
Electroweak symmetry breaking explains the origin of the masses of elementary particles through their interactions with the Higgs field. Besides the measurements of the Higgs boson properties, the study of the scattering of massive vector bosons with spin 1 allows the nature of electroweak symmetry breaking to be probed. Among all processes related to vector-boson scattering, the electroweak production of two jets and a Z-boson pair is a rare and important one. Here we report the observation of this process from proton–proton collision data corresponding to an integrated luminosity of 139 fb−1 recorded at a centre-of-mass energy of 13 TeV with the ATLAS detector at the Large Hadron Collider. We consider two different final states originating from the decays of the Z-boson pair: one containing four charged leptons and another containing two charged leptons and two neutrinos. The hypothesis of no electroweak production is rejected with a statistical significance of 5.7σ, and the measured cross-section for electroweak production is consistent with the Standard Model prediction. In addition, we report cross-sections for inclusive production of a Z-boson pair and two jets for the two final states
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions 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
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
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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
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb−1 of s√ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015–2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z → 4ℓ branching fraction is extracted, giving a value of (4.41 ± 0.30) × 10−6. Constraints on effective field theory parameters and a model based on a spontaneously broken B − L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Search for heavy neutral Higgs bosons produced in association with b-quarks and decaying into b-quarks at root s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Yildiz HD
- Yorita K
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- Zeiner S
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- Zobernig G
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 13/08/2020
- Field of study
A search for heavy neutral Higgs bosons produced in association with one or two
b
-quarks and decaying to
b
-quark pairs is presented using
27.8
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015 and 2016. No evidence of a signal is found. Upper limits on the heavy neutral Higgs boson production cross section times its branching ratio to
b
¯
b
are set, ranging from 4.0 to 0.6 pb at 95% confidence level over a Higgs boson mass range of 450 to 1400 GeV. Results are interpreted within the two-Higgs-doublet model and the minimal supersymmetric Standard Model
- …