455 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
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
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- Whitmore BW
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- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
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- Wolker R
- 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
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- Xiao X
- Xiotidis I
- Xu D
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- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi N
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- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang Y
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- 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 M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- 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 N
- 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
- 01/01/2015
- 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
Evidence-based Kernels: Fundamental Units of Behavioral Influence
- Author
- A Ankjaer-Jensen
- A Appels
- A Biglan
- A Biglan
- A Biglan
- A Biglan
- A Carlsson
- A Hudson
- A Ridgway
- A Robin
- A Rolider
- A Spirito
- A Tanskanen
- A Theodore
- AA Berlin
- AC Wagenaar
- AD Pellegrini
- AD Pellegrini
- AE Kazdin
- AG White
- AH Crisp
- AJ Abramowitz
- AJ Abramowitz
- AJ Richardson
- AK Bay-Hinitz
- AK Dellatan
- AL Dunn
- AL Dunn
- AL Stoll
- AL Stoll
- AL Stoll
- AM Cevasco
- AM Greca la
- AM Hall
- Anthony Biglan
- AP McCain
- AR Cavalier
- AS Matheson
- AS Olafsdottir
- AT Vazsonyi
- AU Rickel
- AW Todd
- AY Mikami
- B Beersma
- B Cabello
- B Egeland
- B Krevor
- B Larsson
- B Law
- B Nemets
- BC Barmann
- BC Barmann
- BC Etzel
- BC McCarty
- BD Winn
- BF Walsh
- BK Martens
- BL Burke
- BR Flay
- BS Cox
- C Choenarom
- C Conyers
- C Conyers
- C Harding
- C Heap
- C Hughes
- C Lonnecker
- C Ostrower
- C Pechmann
- C Pechmann
- C Pechmann
- C Pechmann
- C Schwartz
- C Webster-Stratton
- CA Christle
- CA Ferguson
- CB Ferster
- CB Gesch
- CC Piazza
- CD Adams
- CD Furr-Holden
- CH Hitchcock
- CH Hitchcock
- CH Lawshe
- CH Skinner
- CJ Walker
- CL Harris
- CL Melville
- CL Ringwalt
- CL Storr
- CM Robinson
- CM Saunders
- CN Jacklin
- CR Collier
- CR Greenwood
- CR Greenwood
- CS Green
- CS Lieber
- CV Wilson
- D Barnes
- D Ben Shalom
- D Borfitz
- D Brown
- D Burgess
- D DeMartini-Scully
- D Fletcher
- D Hallfors
- D Hallfors
- D Houlihan
- D McDougall
- D Mischoulon
- D Newbern
- D Newbern
- D Paquette
- D Premack
- D Waard de
- DA Wolfe
- DB Lennox
- DB Shabani
- DB Shabani
- DC Grossman
- DD Embry
- DD Embry
- DD Embry
- DD Embry
- DD Embry
- DD Embry
- DD Hallfors
- DE Wolfe
- Dennis D. Embry
- DF Bjorklund
- DF Dansereau
- DF Dansereau
- DH Allsopp
- DH Schunk
- DH Welsh
- DJ Crews
- DJ Flannery
- DJ Howard
- DK Smith
- DL Schilling
- DL Trammel
- DM Browder
- DM Kamps
- DM Koffman
- DO Rudin
- DP Fry
- DS Pine
- DS Wilson
- DW Blick
- E Atlantis
- E Clark
- E Clark
- E Rodrigues
- E Scott
- EG Krug
- EJ Doyne
- EJ Thomas
- EM Rogers
- ES Geller
- ES Petscher
- ET Hartley
- ET Hartley
- F Jorgensen
- F Juarez
- F Lősel
- F Merrett
- F Scafidi
- FE Hoath
- FJ Silva
- FR Blue
- G Diamond
- G Gaskell
- G Perna
- G Zivin
- GA Fabiano
- GD Sideridis
- GJ Anderson
- GJ DuPaul
- GL Cohen
- GL Schilmoeller
- GM Egeland
- GR Mayer
- GR Mayer
- GS Sorock
- GT Taylor
- GW Joe
- GW Joe
- H Aase
- H Blumenfeld
- H Deutsch
- H Farber
- H Jorgenson
- H Lalramnghinglova
- H Marin
- HA Filcheck
- HA Murphy
- HAC Ninness
- HB Andrews
- HC Ninness
- HH Barrish
- HKM Antunes
- HL Peck
- HM Parsons
- HM Parsons
- HS Henderson
- HS Terrace
- HW Thorpe
- HW Thorpe
- IB Helland
- J Backon
- J Bernstein
- J Derzon
- J Gordon
- J Hevel Van
- J Hill
- J Liu
- J McCambridge
- J Merrett
- J Owusu-Bempah
- J Owusu-Bempah
- J Panksepp
- J Szapocznik
- JA Blumenthal
- JB Barker
- JB Hutton
- JC Delquadri
- JD Shannon
- JE Fishbein
- JE Mazur
- JH Derzon
- JH Sumner
- JJ McCarl
- JJ Priya
- JK Fillingham
- JK Luiselli
- JK Porterfield
- JL Lambert
- JM Campbell
- JM DiFilippo
- JM Ducharme
- JM Ducharme
- JM Ducharme
- JM Ducharme
- JM Ducharme
- JM Ducharme
- JM Leibowitz
- JM Richards
- JM Smyth
- JM Standley
- JM Standley
- JR Boyle
- JR Hibbeln
- JR Hibbeln
- JR Hibbeln
- JR Hibbeln
- JR Hibbeln
- JR Hibbeln
- JR Hibbeln
- JR Hibbeln
- JS Downs
- JS Kahn
- JV Roca
- JW Libb
- JW Maag
- JW Wedel
- K Larson
- K Mishima
- K Nakano
- K Resnicow
- K Spindler
- K Steiner
- K Vaddadi
- K-P Sund
- KA Edwards
- KA Maglieri
- KA Rickards-Schlichting
- KD Lakes
- KE McGoey
- KE Robinson
- KK Kellum
- KL Bledsoe
- KM Greenwood
- KM Hume
- KR Harris
- KT Kivlighan
- KV Naveen
- KW Reagles
- L Chassin
- L Kern
- L Maheady
- L Maheady
- L McDonnell
- L Selznick
- LA Jason
- LA Jason
- LA Jason
- LA Jason
- LA Moore
- LA Pawlow
- LA Sisson
- LAR Stein
- LB Zaichkowsky
- LC Sobell
- LD Allen
- LE Arnold
- LE Arnold
- LE Homme
- LE Melchiori
- LE Possell
- LJ Pfiffner
- LM Saari
- LS Robertson
- LS Robertson
- LV Majovski
- M Agathon
- M Agran
- M Bilici
- M Cook
- M Czuchry
- M Czuchry
- M Czuchry
- M Czuchry
- M Dekovic
- M Fava
- M Gonzalez
- M Haag
- M Heffner
- M Hines
- M Lowndes
- M Marchant
- M Marchant
- M Marion
- M O’Reilly
- M Sherif
- M Sherif
- M Sherif
- M Sherif
- M Sidman
- M Taubman
- M Wolery
- M Wolf
- M-P Leblanc
- MA Bray
- MA Clarke
- MA Diego
- MA Woltersdorf
- MB Medland
- MB Stein
- MC Keel
- MC Luciano
- MC Luciano-Soriano
- MC Roberts
- MC Zanarini
- MJ Boulton
- MJ Ford
- MJ Koepp
- MJ McMorrow
- ML Kelley
- ML McGrath
- ML Rock
- MM Acker
- MM Wolf
- MMR Madaus
- MP Freeman
- MP Freeman
- MR Burch
- MR Dadds
- MR Sanders
- MR Sanders
- MR Sanders
- MS Forgatch
- MS Forgatch
- MS Holloway
- MT Hegel
- MT Palermo
- MW Arthur
- MY Mathes
- N Neave
- N Nicol
- N Ram
- N Rusch
- NA Jones
- NC Jackson
- NK McGrath-Hanna
- NM Hunkin
- NM Petry
- NM Petry
- NM Petry
- NM Petry
- NM Petry
- NM Petry
- NM Petry
- NM Petry
- NN Singh
- NN Singh
- NR Sharma
- NS Gordon
- NS Tobler
- OS Elegbeleye
- OS Jarrett
- P Khatri
- P Palmgreen
- PG Mathes
- PJ Krantz
- PJ Schloss
- PL Ellickson
- PM Fischer
- PM Monti
- PM Stecker
- PN Williamson
- PT Norris
- PW Clement
- PW Dowrick
- PW Dowrick
- R Beyth-Marom
- R Feldman
- R Gardner
- R Gupta
- R Hoigaard
- R Houten Van
- R Houten Van
- R Houten Van
- R Houten Van
- R Jarvinen
- R Leclerc
- R McGee
- R Meadow
- R Nordstrom
- R Nordstrom
- R Sandyk
- R Snell
- RA Block
- RA Davis
- RA Hirasing
- RA Rawson
- RB Reamer
- RC Martella
- RD Abbott
- RE Dustman
- RE Glasgow
- RE Glasgow
- RE Glasgow
- RE Hosford
- RF Putnam
- RG Carey
- RG Harrison
- RJ Cowen
- RJ Sampson
- RM Bell
- RM Foxx
- RM Foxx
- RP Liberman
- RP West
- RS Drabman
- RS Morrison
- RS Ragnarsson
- RV Briscoe
- RW Collins
- S Akhondzadeh
- S Akhtar
- S Erkal
- S Ghosh
- S Gudbjarnason
- S Houghton
- S Kubesch
- S Moore
- S Plummer
- S Rajan
- S Roos
- S Scott
- S Sykes
- S Telles
- SA Godfrey
- SA Stage
- SC Bratton
- SC Carr
- SC Duncan
- SC Hayes
- SC Hayes
- SE Rosenkoetter
- SG Ferber
- SG Kellam
- SG Kellam
- SG Stella
- SI Gray
- SJ Haas-Warner de
- SJ Scholer
- SJ Wood
- SJ Wood
- SK Clare
- SK Wurtele
- SM Burn
- SM Colby
- SM Dees
- SM Ludington-Hoe
- SM Shimabukuro
- SM Siviy
- SP Spera
- SR Eisenstein
- SS Leff
- SS Meharg
- SS Meharg
- ST Ennett
- SW Marshall
- SW Twemlow
- T Bellamy
- T Buggey
- T Buggey
- T Buggey
- T Dalton
- T Field
- T Field
- T Field
- T Field
- T Norlander
- T Ogden
- T Reed
- T Suzuki
- TA Manger
- TD Mickleborough
- TF McLaughlin
- TF McLaughlin
- TH Wang
- TH Wasserman
- TJ Kehle
- TJ Knapp
- TK Taylor
- TL St. Pierre
- TL Stawar
- TM Field
- TM Field
- TN Robinson
- TO Lowe
- TS Ball
- TS Watson
- TW Bean
- TW Hosie
- U Pitre
- U Pitre
- U Pitre
- V Anderson
- V Hertz
- V Sanchez
- VG Spencer
- VL Taylor
- VW Cotter
- W Bennett
- WB Davis
- WR Miller
- WS Agras
- WT Phillips
- XP Chen
- Z Wencai
- Publication venue
- Springer US
- Publication date
- 01/01/2008
- Field of study
This paper describes evidence-based kernels, fundamental units of behavioral influence that appear to underlie effective prevention and treatment for children, adults, and families. A kernel is a behavior–influence procedure shown through experimental analysis to affect a specific behavior and that is indivisible in the sense that removing any of its components would render it inert. Existing evidence shows that a variety of kernels can influence behavior in context, and some evidence suggests that frequent use or sufficient use of some kernels may produce longer lasting behavioral shifts. The analysis of kernels could contribute to an empirically based theory of behavioral influence, augment existing prevention or treatment efforts, facilitate the dissemination of effective prevention and treatment practices, clarify the active ingredients in existing interventions, and contribute to efficiently developing interventions that are more effective. Kernels involve one or more of the following mechanisms of behavior influence: reinforcement, altering antecedents, changing verbal relational responding, or changing physiological states directly. The paper describes 52 of these kernels, and details practical, theoretical, and research implications, including calling for a national database of kernels that influence human behavior
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- 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
- Aperio Bella L
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azoulay AM
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Bakshi Gupta D
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
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- Zhemchugov A
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- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Prognostic model to predict postoperative acute kidney injury in patients undergoing major gastrointestinal surgery based on a national prospective observational cohort study.
- Author
- Aamir A
- Abbas J
- Abbas N
- Abbott TEF
- Abdalla M
- Abdikadir H
- Abuhussein N
- Acquaah F
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- STARSurg Collaborative Writing Committee, Data analysis, Steering committee, Advisory group, Regional leads, Collaborators and validators
- STARSurg Collaborative Writing Committee, Data analysis, Steering committee, Advisory group, Regional leads, Collaborators and validators, Nepogodiev, D
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- Zubikarai G
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- Publication venue
- 'Wiley'
- Publication date
- 18/05/2018
- Field of study
Background: Acute illness, existing co-morbidities and surgical stress response can all contribute to postoperative acute kidney injury (AKI) in patients undergoing major gastrointestinal surgery. The aim of this study was prospectively to develop a pragmatic prognostic model to stratify patients according to risk of developing AKI after major gastrointestinal surgery. Methods: This prospective multicentre cohort study included consecutive adults undergoing elective or emergency gastrointestinal resection, liver resection or stoma reversal in 2-week blocks over a continuous 3-month period. The primary outcome was the rate of AKI within 7 days of surgery. Bootstrap stability was used to select clinically plausible risk factors into the model. Internal model validation was carried out by bootstrap validation. Results: A total of 4544 patients were included across 173 centres in the UK and Ireland. The overall rate of AKI was 14·2 per cent (646 of 4544) and the 30-day mortality rate was 1·8 per cent (84 of 4544). Stage 1 AKI was significantly associated with 30-day mortality (unadjusted odds ratio 7·61, 95 per cent c.i. 4·49 to 12·90; P < 0·001), with increasing odds of death with each AKI stage. Six variables were selected for inclusion in the prognostic model: age, sex, ASA grade, preoperative estimated glomerular filtration rate, planned open surgery and preoperative use of either an angiotensin-converting enzyme inhibitor or an angiotensin receptor blocker. Internal validation demonstrated good model discrimination (c-statistic 0·65). Discussion: Following major gastrointestinal surgery, AKI occurred in one in seven patients. This preoperative prognostic model identified patients at high risk of postoperative AKI. Validation in an independent data set is required to ensure generalizability
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
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- Calace N
- Calafiura P
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- Carrillo-Montoya GD
- Casadei D
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- 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
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- Yao W-M
- Yap YC
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- 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
Measurement of Azimuthal Anisotropy of Muons from Charm and Bottom Hadrons 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
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
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- Adamczyk L
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- Agheorghiesei C
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- Capeans Garrido MDM
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- Capua M
- Carbone RM
- Cardarelli R
- Cardillo FC
- Carli I
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- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 28/02/2020
- Field of study
The elliptic flow of muons from the decay of charm and bottom hadrons is measured in
p
p
collisions at
√
s
=
13
TeV
using a data sample with an integrated luminosity of
150
pb
−
1
recorded by the ATLAS detector at the LHC. The muons from heavy-flavor decay are separated from light-hadron decay muons using momentum imbalance between the tracking and muon spectrometers. The heavy-flavor decay muons are further separated into those from charm decay and those from bottom decay using the distance-of-closest-approach to the collision vertex. The measurement is performed for muons in the transverse momentum range 4–7 GeV and pseudorapidity range
|
η
|
<
2.4
. A significant nonzero elliptic anisotropy coefficient
v
2
is observed for muons from charm decays, while the
v
2
value for muons from bottom decays is consistent with zero within uncertainties
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
- AbouZeid OS
- Abraham NL
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- Yildiz HD
- Yorita K
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- Zaripovas DR
- Zeiner S
- Zeitnitz C
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- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
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- Zhang Z
- Zhang Z
- Zhao P
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu CG
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- 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
- 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
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
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
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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
Observation of Electroweak Production of a Same-Sign W Boson Pair in Association with Two Jets in pp Collisions root s=13 TeV with the ATLAS Detector
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- Zhemchugov A
- Zheng Z
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- Zibell A
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- Zinonos Z
- Zinser M
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- Zivkovic L
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zur Nedden M
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 18/10/2019
- Field of study
This Letter presents the observation and measurement of electroweak production of a same-sign
W
boson pair in association with two jets using
36.1
fb
−
1
of proton-proton collision data recorded at a center-of-mass energy of
√
s
=
13
TeV
by the ATLAS detector at the Large Hadron Collider. The analysis is performed in the detector fiducial phase-space region, defined by the presence of two same-sign leptons, electron or muon, and at least two jets with a large invariant mass and rapidity difference. A total of 122 candidate events are observed for a background expectation of
69
±
7
events, corresponding to an observed signal significance of 6.5 standard deviations. The measured fiducial signal cross section is
σ
fid
=
2.89
+
0.51
−
0.48
(
stat
)
+
0.29
−
0.28
(
syst
)
fb
Search for excited electrons singly produced in proton–proton collisions at \sqrt{s} = 13 TeV with the ALAS experiment at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- 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
- Arabidze G
- Aranda CP
- Araque JP
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Artamonov A
- Artoni G
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- Asimakopoulou EM
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- Zhemchugov A
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- Zhulanov V
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- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2019
- Field of study
A search for excited electrons produced in pp collisions at s√ = 13 TeV via a contact interaction qq¯→ee∗ is presented. The search uses 36.1 fb −1 of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron into an electron and a pair of quarks ( eqq¯ ) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a W boson ( νW ) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying W boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the pp→ee∗→eeqq¯ and pp→ee∗→eνW production cross sections as a function of the excited electron mass me∗ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter Λ of the model as a function of me∗ . For me∗<0.5 TeV , the lower bound for Λ is 11 TeV . In the special case of me∗=Λ , the values of me∗<4.8 TeV are excluded. The presented limits on Λ are more stringent than those obtained in previous searches
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