238 research outputs found
Overlap of cognitive concepts in chronic widespread pain: An exploratory study
- Author
- A Bandura
- A Köke
- A Luszczynska
- A Miles
- A Williamson
- AK Rosenstiel
- Aleid de Rooij
- AT Beck
- C Mounce
- CP Van Wilgen
- CS Burckhardt
- DC Turk
- DC Turk
- E Denison
- E Denison
- E Fernandez
- F Wolfe
- FJ Keefe
- G Crombez
- GK Brown
- H Leventhal
- H Leventhal
- H Merskey
- J Lethem
- J Roelofs
- J Weinman
- JA Turner
- JA Turner
- JM Bland
- JM Lacker
- Joke A Vollebregt
- Joost Dekker
- JW Reich
- JW Vlaeyen
- K Lawson
- K Mannerkorpi
- L Goubert
- LC Barry
- LD Cameron
- Leo D Roorda
- M Leeuw
- MA Davidson
- Martijn PM Steultjens
- ME Robinson
- MJWM Heijmans
- MK Nicholas
- MP Jensen
- MP Jensen
- MS Hagger
- MW Van Ittersum
- P Arnstein
- P Spinhoven
- Petra C Siemonsma
- R Moss-Morris
- R Schwarzer
- RS Lazarus
- SF Mikail
- SP Buckelew
- SP Buckelew
- TA De Gagne
- U Scholz
- Willemine Beuving
- WJ Taylor
- WR Nielson
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>A wide variety of cognitive concepts have been shown to play an important role in chronic widespread pain (CWP). Although these concepts are generally considered to be distinct entities, some might in fact be highly overlapping. The objectives of this study were to (i) to establish inter-relationships between self-efficacy, cognitive coping styles, fear-avoidance cognitions and illness beliefs in patients with CWP and (ii) to explore the possibility of a reduction of these cognitions into a more limited number of domains.</p> <p>Methods</p> <p>Baseline measurement data of a prospective cohort study of 138 patients with CWP were used. Factor analysis was used to study the associations between 16 different cognitive concepts.</p> <p>Results</p> <p>Factor analysis resulted in three factors: 1) negative emotional cognitions, 2) active cognitive coping, and 3) control beliefs and expectations of chronicity.</p> <p>Conclusion</p> <p>Negative emotional cognitions, active cognitive coping, control beliefs and expectations of chronicity seem to constitute principal domains of cognitive processes in CWP. These findings contribute to the understanding of overlap and uniqueness of cognitive concepts in chronic widespread pain.</p
Caveats of chronic exogenous corticosterone treatments in adolescent rats and effects on anxiety-like and depressive behavior and hypothalamic-pituitary-adrenal (HPA) axis function
- Author
- AE Pekary
- AE Ryabinin
- AL Lussier
- AM Bao
- AM Barr
- AM Magarinos
- B Lee
- C Mathers
- C Rockhill
- C Woolley
- CD Allen
- CD Allen
- CD Conrad
- CD Conrad
- CL Parks
- CM McCormick
- CM McCormick
- CM McCormick
- CM McCormick
- CM McCormick
- CM McCormick
- CM McCormick
- CM Pariante
- DA Tata
- DD Rasmussen
- DH Overstreet
- DJ David
- DP Cantwell
- E Brown
- E Karanges
- E Tirelli
- EA Stone
- EA Stone
- EY Sterner
- FW Ellis
- H Anisman
- HA Cameron
- IZ Mathews
- J Haller
- J Izumi
- J Nacher
- J Wang
- JF Cryan
- JF Cryan
- JW Richardson-Jones
- K Beesdo
- KE Grant
- KM Ogilvie
- LD Dorn
- LE Kalynchuk
- LE Reardon
- LP Spear
- LP Spear
- MD Morrissey
- MM Przybycien-Szymanska
- MM Silveri
- N Risch
- N Sousa
- P Willner
- PM Wall
- R McArthur
- RC Kessler
- RD Porsolt
- RF Genn
- S Pellow
- SA Johnson
- SL Gourley
- SM Paul
- T Enkel
- T Pung
- TL Doremus
- TS Perrot-Sinal
- V Castagne
- W Marks
- WC Drevets
- Y Watanabe
- YJG Karten
- Z Xu
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Administration of exogenous corticosterone is an effective preclinical model of depression, but its use has involved primarily adult rodents. Using two different procedures of administration drawn from the literature, we explored the possibility of exogenous corticosterone models in adolescence, a time of heightened risk for mood disorders in humans.</p> <p>Methods</p> <p>In experiment 1, rats were injected with 40 mg/kg corticosterone or vehicle from postnatal days 30 to 45 and compared with no injection controls on behavior in the elevated plus maze (EPM) and the forced swim test (FST). Experiment 2 consisted of three treatments administered to rats from postnatal days 30 to 45 or as adults (days 70 to 85): either corticosterone (400 μg/ml) administered in the drinking water along with 2.5% ethanol, 2.5% ethanol or water only. In addition to testing on EPM, blood samples after the FST were obtained to measure plasma corticosterone. Analysis of variance (ANOVA) and alpha level of <it>P </it>< 0.05 were used to determine statistical significance.</p> <p>Results</p> <p>In experiment 1, corticosterone treatment of adolescent rats increased anxiety in the EPM and decreased immobility in the FST compared to no injection control rats. However, vehicle injected rats were similar to corticosterone injected rats, suggesting that adolescent rats may be highly vulnerable to stress of injection. In experiment 2, the intake of treated water, and thus doses delivered, differed for adolescents and adults, but there were no effects of treatment on behavior in the EPM or FST. Rats that had ingested corticosterone had reduced corticosterone release after the FST. Ethanol vehicle also affected corticosterone release compared to those ingesting water only, but differently for adolescents than for adults.</p> <p>Conclusions</p> <p>The results indicate that several challenges must be overcome before the exogenous corticosterone model can be used effectively in adolescents.</p
A922 Sequential measurement of 1 hour creatinine clearance (1-CRCL) in critically ill patients at risk of acute kidney injury (AKI)
- Author
- Abbott TE
- Abdallah RI
- Abdel-Aal IR
- Abdelmonem SA
- Abdo WF
- Abellan AN
- Abellán AN
- Abellán AN
- Abellán AN
- Abrams ST
- Ackerley C
- Acuña M
- Adda M
- Adhikari NK
- Adriano G
- Adrie C
- Affatato R
- Affatato R
- Afonso-Rivero D
- Agarossi A
- Agarwal LK
- Ageeva T
- Agrawal R
- Aguayo-DeHoyos E
- Aguilar AL
- Aguilar-Alonso E
- Aguilar-Alonso E
- Aguilar-Alonso E
- Aguirregabyria M
- Ahmadnia E
- Ahn C
- Ahn JY
- Ahn JY
- Ahn MY
- Ahn MY
- Aitken LM
- Akalaev R
- Akbarzadeh A
- Akcan-Arikan A
- Akhlagh SH
- Akhtar N
- AKI Research Group
- Akiduki N
- Akin S
- Akizuki N
- Akkoc T
- Ala-Kokko T
- Alanio A
- Albaiceta GM
- Albaladejo P
- Alberto F
- Albuisson E
- Alcala MA
- Alcázar L
- Aldabo-Pallas T
- Aldana NN
- Aldecoa C
- Alegría L
- Alejandro R
- Alejo GC
- Alejos RM
- Alexandrova E
- Algarte R
- Algarte R
- Algieri I
- Algora-Weber A
- Alhamdi Y
- Aliaga FA
- Aliberti S
- Alkan A
- Almudena PM
- Almudevar PM
- Almudevar PM
- Almudévar PM
- Altıntas ND
- Alvarez J
- Alves SC
- Alzola LM
- Amargianitakis V
- Amaro R
- Amato MB
- Ambler M
- Amerongen MP
- Amininejad T
- Amor LL
- Amorim V
- Anand RK
- Andersen LW
- Andersson S
- Andoh K
- Andrade AH
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- Andrade G
- Andreis DT
- Andreis DT
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- Antonelli M
- Antoniadou A
- Antonio C
- Antonucci E
- Antón DG
- Anzueto A
- Appiani F
- Aquevedo A
- Aragon C
- Araujo NJ
- Araujo VF
- ARIAM registry of adult cardiac surgery
- ARIAM-ANDALUCIA
- Arias CC
- Arias N
- Arias-Verdu MD
- Arias-Verdu MD
- Arias-Verdu MD
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- Arslantas MK
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- Avilés-Jurado FX
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- Ayala LY
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- Azevedo JC
- Azevedo JR
- Aznar GP
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- Banderas-Bravo ME
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- Charitidou E
- Charpentier C
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- Chen CM
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- Cheng CC
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- Chernyshuk S
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- Chhor V
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- FINNRESUSCI Study Group
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- Hatib F
- Hawkins K
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- Hayakawa M
- Hayakawa M
- Hayakawa M
- Hayakawa M
- Hayashi K
- He X
- Healey AJ
- Hebert P
- Hegazy S
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- Helmy TA
- Helyar S
- Helyar S
- Hempel D
- Henderson MA
- Hendra H
- Henschel B
- Heras G
- Hernandis V
- Hernández A
- Hernández AA
- Hernández AA
- Hernández AA
- Hernández AA
- Hernández AA
- Hernández AA
- Hernández G
- Hernández-Tejedor A
- Herpain A
- Herrera AN
- Herrera AN
- Herrera AN
- Herrera AN
- Herrera AN
- Herrera AN
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- Heunks LM
- Hewitt H
- Heyne T
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- Hidalgo C
- Hikasa Y
- Hillier SD
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- Himpe D
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- Hirata A
- Hirayama T
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- Hodgson LE
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- Houzé S
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- Hraiech S
- Hravnak M
- Hu HC
- Hua Y
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- Hualde JB
- Hualde JB
- Hualde JB
- Hualde JB
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- Huang CH
- Huang WC
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- Huang WC
- Huang WC
- Hubbard A
- Huber W
- Huddart S
- Hull AM
- Hung CY
- Hung WT
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- Huot B
- Husheer SL
- Hutchings S
- Hutchison R
- Hwang GS
- Hwang GS
- Ibañes PG
- Ibsen M
- Idei M
- Idei M
- Idone FA
- Iesu E
- Iesu E
- Iglesias-Santiago A
- Ignacio ML
- Iida A
- Iijima H
- Ilan R
- Ilyina V
- Imanaka H
- Inaloo S
- Ince C
- Iotti GA
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- IPREA Study Group
- Irazabal JM
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- Itenov TS
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- Jacobs FM
- Jacques T
- Jaffal K
- Jamali S
- Jang BH
- Janotka M
- Janotka M
- Janotka M
- Jansen D
- Jansen N
- Japan Septic Disseminated Intravascular Coagulation (JSEPTIC DIC) study group
- Jardim JJ
- Jardim M
- Jareño A
- Javadpour S
- Jayasinghe S
- Jean-Baptiste S
- Jean-Baptiste S
- Jensen AE
- Jensen JU
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- Jeon YD
- Jeong IY
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- Jian Z
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- Jiménez GJ
- Jo YH
- Joachim J
- Jochmans S
- John G
- Jonas M
- Jonas M
- Jonas M
- Jones C
- Joshi R
- Joshi V
- Jovaisa T
- JSEPTIC (Japanese Society of Education for Physicians and Trainees in Intensive Care) Clinical Trial Group
- Juan WC
- Juanas CA
- Judickas S
- Juez A
- Juliarena A
- Jun IG
- Jun IG
- Jung K
- Jung KW
- Junior JM
- Kaczirek K
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- Kalenka A
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- Kamali E
- Kaminsky GE
- Kaneko M
- Kang M
- Kang M
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- Kang PL
- Kang PL
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- Kang Y
- Kao KC
- Kappler F
- Kara A
- Karachi F
- Karanjia N
- Karbing DS
- Karsten E
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- Kashiya S
- Kashyap R
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- Katabami K
- Katabami K
- Katabami K
- Katira BH
- Kavanagh BP
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- Kawano S
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- Kayaaslan B
- Kayambu G
- Kazutoshi F
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- Kim DJ
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- Kim MH
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- Kim W
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- Kirakli C
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- Kirwan CJ
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- Kleinpell R
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- Knafelj R
- Knight LD
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- Ko SB
- Kobayashi A
- Koco E
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- Kodate A
- Kodate A
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- Kolnikova I
- Komuro T
- Kondili E
- Kongpolprom N
- Kooner G
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- Kosuk ME
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- Kou PS
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- Kox M
- Kraegpoeth A
- Krenn CG
- Krishna B
- Kristof J
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- Kruger A
- Krüger A
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- Kubota K
- Kuebler WM
- Kulaga EV
- Kulkarni AP
- Kumari BK
- Kumbamu A
- Kunze-Szikszay N
- Kurmukov IA
- Kurth T
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- Kurtz P
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- Kwon HM
- Kwon WY
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- Labra C
- Lacerda P
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- Lafuente E
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- Lagos R
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- Latini R
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- Lichtenstein D
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- Lin WC
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- Lischinsky A
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- Lombardo MD
- Londoño JG
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- Lukaszewicz AC
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- Merino-Vega D
- Messenger D
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- Okayama Research Investigation Organizing Network (ORION)investigators
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- Álvarez JT
- Álvarez-Lerma F
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Meeting abstrac
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
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- Abusleme Hoffman AC
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- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhou Y
- Zhu CG
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- Zhu Y
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Search for pair production of squarks or gluinos decaying via sleptons or weak bosons in final states with two same-sign or three leptons with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
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- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi A
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- Ali B
- Ali HMJ
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- Alibocus SW
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- Alkakhi W
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- Allbrooke BMM
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- Allendes Flores CA
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- Alviggi MG
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 15/02/2024
- Field of study
A search for pair production of squarks or gluinos decaying via sleptons or weak bosons is reported. The search targets a final state with exactly two leptons with same-sign electric charge or at least three leptons without any charge requirement. The analysed data set corresponds to an integrated luminosity of 139 fb−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Multiple signal regions are defined, targeting several SUSY simplified models yielding the desired final states. A single control region is used to constrain the normalisation of the WZ + jets background. No significant excess of events over the Standard Model expectation is observed. The results are interpreted in the context of several supersymmetric models featuring R-parity conservation or R-parity violation, yielding exclusion limits surpassing those from previous searches. In models considering gluino (squark) pair production, gluino (squark) masses up to 2.2 (1.7) TeV are excluded at 95% confidence level
All-sky, all-frequency directional search for persistent gravitational waves from Advanced LIGO’s and Advanced Virgo’s first three observing runs
- Author
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- Zhu Z-H
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 03/06/2022
- Field of study
We present the first results from an all-sky all-frequency (ASAF) search for
an anisotropic stochastic gravitational-wave background using the data from the
first three observing runs of the Advanced LIGO and Advanced Virgo detectors.
Upper limit maps on broadband anisotropies of a persistent stochastic
background were published for all observing runs of the LIGO-Virgo detectors.
However, a broadband analysis is likely to miss narrowband signals as the
signal-to-noise ratio of a narrowband signal can be significantly reduced when
combined with detector output from other frequencies. Data folding and the
computationally efficient analysis pipeline, {\tt PyStoch}, enable us to
perform the radiometer map-making at every frequency bin. We perform the search
at 3072 {\tt{HEALPix}} equal area pixels uniformly tiling the sky and in every
frequency bin of width 1/32~Hz in the range 20−1726~Hz, except for bins
that are likely to contain instrumental artefacts and hence are notched. We do
not find any statistically significant evidence for the existence of narrowband
gravitational-wave signals in the analyzed frequency bins. Therefore, we place
95% confidence upper limits on the gravitational-wave strain for each
pixel-frequency pair, the limits are in the range (0.030−9.6)×10−24. In addition, we outline a method to identify candidate
pixel-frequency pairs that could be followed up by a more sensitive (and
potentially computationally expensive) search, e.g., a matched-filtering-based
analysis, to look for fainter nearly monochromatic coherent signals. The ASAF
analysis is inherently independent of models describing any spectral or spatial
distribution of power. We demonstrate that the ASAF results can be
appropriately combined over frequencies and sky directions to successfully
recover the broadband directional and isotropic results
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Aakvaag E
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboelela M
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Ackermann A
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Aktas S
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Alegria ZL
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi F
- Algren M
- Alhroob M
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- Ali HMJ
- Ali S
- Alibocus SW
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- Allaire C
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- Alviggi MG
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- Amirie KJ
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- Zhang Y
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- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhu CG
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- Zhu Y
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- Zhuang X
- Zhukov K
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Performance and calibration of quark/gluon-jet taggers using 140 fb⁻¹ of pp collisions at √s=13 TeV with the ATLAS detector
- Author
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- Abbott B
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- Abidi SH
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- Zhemchugov A
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/02/2024
- Field of study
The identification of jets originating from quarks and gluons, often referred to as quark/gluon tagging,
plays an important role in various analyses performed at the Large Hadron Collider, as Standard Model measurements and searches for new particles decaying to quarks often rely on suppressing a large gluon-induced background. This paper describes the measurement of the efficiencies of quark/gluon taggers developed within the ATLAS Collaboration, using √s=13 TeV proton–proton collision data with an integrated luminosity of 140 fb-1 collected by the ATLAS experiment. Two taggers with high performances in rejecting jets from gluon over jets from
quarks are studied: one tagger is based on requirements on the number of inner-detector tracks associated with the
jet, and the other combines several jet substructure observables using a boosted decision tree. A method is established to determine the quark/gluon fraction in data, by using quark/gluon-enriched subsamples defined by the jet
pseudorapidity. Differences in tagging efficiency between data and simulation are provided for jets with transverse
momentum between 500 GeV and 2 TeV and for multiple tagger working points
Search for resonant production of dark quarks in the dijet final state with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
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- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
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- Alegria ZL
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- Aleksandrov IN
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- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
- Zhang DF
- Zhang J
- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/02/2024
- Field of study
This paper presents a search for a new Z′ resonance decaying into a pair of dark quarks which hadronise into dark hadrons before promptly decaying back as Standard Model particles. This analysis is based on proton-proton collision data recorded at s
s
= 13 TeV with the ATLAS detector at the Large Hadron Collider between 2015 and 2018, corresponding to an integrated luminosity of 139 fb−1. After selecting events containing large-radius jets with high track multiplicity, the invariant mass distribution of the two highest-transverse-momentum jets is scanned to look for an excess above a data-driven estimate of the Standard Model multijet background. No significant excess of events is observed and the results are thus used to set 95% confidence-level upper limits on the production cross-section times branching ratio of the Z′ to dark quarks as a function of the Z′ mass for various dark-quark scenarios
Electron and photon energy calibration with the ATLAS detector using LHC Run 2 data
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
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- Acharya BS
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- Zhemchugov A
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- Zhulanov V
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- Ziolkowski M
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/02/2024
- Field of study
This paper presents the electron and photon energy calibration obtained with the ATLAS detector using 140 fb-1 of LHC proton-proton collision data recorded at √(s) = 13 TeV between 2015 and 2018. Methods for the measurement of electron and photon energies are outlined, along with the current knowledge of the passive material in front of the ATLAS electromagnetic calorimeter. The energy calibration steps are discussed in detail, with emphasis on the improvements introduced in this paper. The absolute energy scale is set using a large sample of Z-boson decays into electron-positron pairs, and its residual dependence on the electron energy is used for the first time to further constrain systematic uncertainties. The achieved calibration uncertainties are typically 0.05% for electrons from resonant Z-boson decays, 0.4% at ET ∼ 10 GeV, and 0.3% at ET ∼ 1 TeV; for photons at ET ∼ 60 GeV, they are 0.2% on average. This is more than twice as precise as the previous calibration. The new energy calibration is validated using J/ψ → ee and radiative Z-boson decays
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