270 research outputs found
Validation of the surgical fear questionnaire in adult patients waiting for elective surgery
- Author
- A Boker
- A Dihle
- A Shafer
- AS Zigmond
- Audrey A. A. Fiddelers
- CD Spielberger
- E Carr
- EL Poleshuck
- Erik G. W. Schouten
- Hans-Fritz Gramke
- HF Gramke
- I Bjelland
- Jeremy Miles
- JL Riley
- K Millar
- KI de Groot
- KW Ene
- L Hu
- LE Graham
- M Johnston
- M Johnston
- M Koivula
- M Koivula
- M Sommer
- M Sommer
- M Theunissen
- M Zieger
- MA Ferreira-Valente
- Madelon L. Peters
- Marco A. E. Marcus
- Mark G. A. Willemsen
- Maurice Theunissen
- MJL Sullivan
- ML Peters
- ML Peters
- MR Munafo
- N Moerman
- Patrícia R. Pinto
- PH Rosenberger
- PR Pinto
- PR Pinto
- S Van Damme
- SV Kleinbeck
- V Graver
- W Caumo
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2014
- Field of study
Objectives: Because existing instruments for assessing surgical fear seem either too general or too limited, the Surgical Fear Questionnaire (SFQ) was developed. The aim of this study is to assess the validity and reliability of the SFQ.
Methods: Based on existing literature and expert consultation the ten-item SFQ was composed. Data on the SFQ were obtained from 5 prospective studies (N = 3233) in inpatient or day surgery patients. These data were used for exploratory factor analysis (EFA), confirmatory factor analysis (CFA), reliability analysis and validity analysis.
Results: EFA in Study 1 and 2 revealed a two-factor structure with one factor associated with fear of the short-term consequences of surgery (SFQ-s, item 1-4) and the other factor with fear of the long-term consequences of surgery (SFQ-l, item 5-10). However, in both studies two items of the SFQ-l had low factor loadings. Therefore in Study 3 and 4 the 2-factor structure was tested and confirmed by CFA in an eight-item version of the SFQ. Across all studies significant correlations of the SFQ with pain catastrophizing, state anxiety, and preoperative pain intensity indicated good convergent validity. Internal consistency (Cronbach's alpha) was between 0.765-0.920 (SFQ-total), 0.766-0.877 (SFQ-s), and 0.628-0.899 (SFQ-l). The SFQ proved to be sensitive to detect differences based on age, sex, education level, employment status and preoperative pain intensity.
Discussion: The SFQ is a valid and reliable eight-item index of surgical fear consisting of two subscales: fear of the short-term consequences of surgery and fear of the long-term consequences.This study was conducted with departmental funding and supported by a grant from The Netherlands Organisation for Scientific Research (Zon-MW, http://www.zonmw.nl/en/), grant no. 110000007. The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript
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
- 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
- Aikot A
- Ait Tamlihat M
- 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
- Alexopoulos T
- Alfonsi F
- Algren M
- Alhroob M
- Ali B
- Ali HMJ
- Ali S
- Alibocus SW
- Aliev M
- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allen JF
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
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- Ambler A
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- Ames CG
- Amidei D
- Amor Dos Santos SP
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- Ananiev V
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- 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
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- Nickerson RB
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- Okumura Y
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- Olivares Pino SA
- Oliveira Damazio D
- Oliveira Goncalves D
- Oliver JL
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- Onyisi PUE
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- Padilla Aranda C
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- Piazza F
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- Pinfold JL
- Pinheiro Pereira BC
- Pinto Pinoargote AE
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- Plesanovs V
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- Riu I
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- Robles Gajardo CM
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- Robson A
- Rocchi A
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- Rodriguez Garcia Y
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- Romero Hernandez AC
- Rompotis N
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- Rozanov A
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- Ruby AJ
- Ruelas Rivera VH
- Ruggeri TA
- Ruggiero A
- Ruiz-Martinez A
- Rummler A
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- Rusakovich NA
- Russell HL
- Russo G
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- Schumacher M
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- Schäfer U
- Sciandra A
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- Sebastiani CD
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- Seema P
- Seidel SC
- Seiden A
- Seidlitz BD
- Seitz C
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- Sekula SJ
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- Sengupta D
- Senthilkumar V
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sforza F
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- Shabalina E
- Shaheen R
- Shahinian JD
- Shaked Renous D
- Shan LY
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- Sharma A
- Sharma AS
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- Shimmin CO
- Shimogama Y
- Shinner JD
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
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- Shojaii J
- Shope DR
- Shrestha B
- Shrestha S
- Shrif EM
- Shroff MJ
- Sicho P
- Sickles AM
- Sideras Haddad E
- Sidoti A
- Siegert F
- Sijacki Dj
- Sikora R
- Sili F
- Silva Oliveira MV
- Silva JM
- Silverstein SB
- Simion S
- Simoniello R
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- Sindhu S
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- Sivoklokov S Yu
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- Smart BH
- Smiesko J
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- Smirnov Y
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- Snesarev AA
- Snider SR
- Snoek HL
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- Sobie R
- Soffer A
- Solans Sanchez CA
- Soldatov E Yu
- Soldevila U
- Solodkov AA
- Solomon S
- Soloshenko A
- Solovieva K
- Solovyanov OV
- Solovyev V
- Sommer P
- Sonay A
- Song WY
- Sonneveld JM
- Sopczak A
- Sopio AL
- Sopkova F
- Sothilingam V
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- Soualah R
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- South D
- Spagnolo S
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- Spigo G
- Spina M
- Spinali S
- Spiteri DP
- Spousta M
- Staats EJ
- Stabile A
- Stamen R
- Stamenkovic M
- Stampekis A
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- Stanecka E
- Stange MV
- Stanislaus B
- Stanitzki MM
- Stapf B
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- Sulin VV
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- Sultanaliyeva L
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- Sun S
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- Suzuki H
- Svatos M
- Swiatlowski M
- Swirski T
- Sykora I
- Sykora M
- Sykora T
- Sánchez J
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Tafoya Vargas JS
- Takeva EP
- Takubo Y
- Talby M
- Talyshev AA
- Tam KC
- Tamir NM
- Tanaka A
- Tanaka J
- Tanaka R
- Tanasini M
- Tao Z
- Tapia Araya S
- Tapprogge S
- Tarek Abouelfadl Mohamed A
- Tarem S
- Tariq K
- Tarna G
- Tartarelli GF
- Tas P
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- Tayalati Y
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- Teixeira-Dias P
- Teoh JJ
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Thaler A
- The ATLAS collaboration
- Theiner O
- Themistokleous N
- Theveneaux-Pelzer T
- Thielmann O
- Thomas DW
- Thomas JP
- Thompson EA
- Thompson PD
- Thomson E
- Tian Y
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- Togawa M
- Tojo J
- Tokushuku K
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- Tomoto M
- Tompkins L
- Topolnicki KW
- Torrence E
- Torres H
- Torró Pastor E
- Toscani M
- Tosciri C
- Tost M
- Tovey DR
- Traeet A
- Trandafir IS
- Trefzger T
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Trischuk DA
- Trocmé B
- Troncon C
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tsai M
- Tsiamis A
- Tsiareshka PV
- Tsigaridas S
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsujikawa Y
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsur O
- Tsuri K
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna AN
- Turchikhin S
- Turk Cakir I
- Turra R
- Turtuvshin T
- Tuts PM
- Tzamarias S
- Tzanis P
- Tzovara E
- Uchida K
- Ukegawa F
- Ulloa Poblete PA
- Umaka EN
- Unal G
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- Undrus A
- Unel G
- Urban J
- Urquijo P
- Usai G
- Ushioda R
- Usman M
- Uysal Z
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vafeiadis T
- Vaitkus A
- Valderanis C
- Valdes Santurio E
- Valente M
- Valentinetti S
- Valero A
- Valiente Moreno E
- Vallier A
- Valls Ferrer JA
- Van Arneman DR
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- Van Der Graaf A
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- Van Vulpen I
- Vanadia M
- Vandelli W
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- Vandewall ER
- Vannicola D
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- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varriale L
- Varvell KE
- Vasile ME
- Vaslin L
- Vasquez GA
- Vazeille F
- Vazquez Schroeder T
- Veatch J
- Vecchio V
- Veen MJ
- Veliscek I
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Verbytskyi A
- Verducci M
- Vergis C
- Verissimo De Araujo M
- Verkerke W
- Vermeulen JC
- Vernieri C
- Vessella M
- Vetterli MC
- Vgenopoulos A
- Vickey Boeriu OE
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Villaplana Perez M
- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Visibile A
- Vittori C
- Vivarelli I
- Vladimirov V
- Voevodina E
- Vogel F
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- Von Ahnen J
- Von Toerne E
- Vormwald B
- Vorobel V
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- Vozdecky L
- Vranjes Milosavljevic M
- Vranjes N
- Vreeswijk M
- Vuillermet R
- Vujinovic O
- Vukotic I
- Wada S
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- Wahdan S
- Wahlberg H
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- Walder J
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- Walkowiak W
- Wall A
- Wamorkar T
- Wang AZ
- Wang C
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- Wang R
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- Wang S
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- Wang WT
- Wang X
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- Warburton A
- Ward RJ
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- Wei C
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- Weidberg AR
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- Weingarten J
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- Wells CJ
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- Wendland B
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- Wessels M
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- Whiteson D
- Wickremasinghe L
- Wiedenmann W
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- Wiglesworth C
- Wilbern DJ
- Wilkens HG
- Williams DM
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- Williams S
- Willocq S
- Wilson BJ
- Windischhofer PJ
- Winkel FI
- Winklmeier F
- Winter BT
- Winter JK
- Wittgen M
- Wobisch M
- Wolffs Z
- Wollrath J
- Wolter MW
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- Wongel AF
- Worm SD
- Wosiek BK
- Wozniewski S
- Woźniak KW
- Wraight K
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- Wu M
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- Wu SL
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- Wu Y
- Wu Z
- Wuerzinger J
- Wyatt TR
- Wynne BM
- Wölker R
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- Xiang J
- Xiao X
- Xie M
- Xie X
- Xin S
- Xiong J
- Xu D
- Xu H
- Xu L
- Xu R
- Xu T
- Xu Y
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yamaguchi N
- Yamaguchi Y
- Yamashita E
- Yamauchi H
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan S
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang X
- Yang Y
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Ye H
- Ye H
- Ye J
- Ye S
- Ye X
- Yeh Y
- Yeletskikh I
- Yeo BK
- Yexley MR
- Yin P
- Yorita K
- Younas S
- Young C
- Young CJS
- Yu Y
- Yuan M
- Yuan R
- Yue L
- Zaazoua M
- Zabinski B
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
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- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- 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
- 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
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
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- Zhemchugov A
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- Zimine NI
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- 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
Software Performance of the ATLAS Track Reconstruction for LHC Run 3
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- Abidi SH
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- Yue L
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- Zabinski B
- Zagazeta LF Gutierrez
- Zaid E
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- Zakharchuk N
- Zambito S
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
- Zhai M
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- Zhang R
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- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- 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
- 02/04/2024
- Field of study
Charged particle reconstruction in the presence
of many simultaneous proton–proton (pp) collisions in the
LHC is a challenging task for the ATLAS experiment’s reconstruction software due to the combinatorial complexity. This
paper describes the major changes made to adapt the software
to reconstruct high-activity collisions with an average of 50 or
more simultaneous pp interactions per bunch crossing (pileup) promptly using the available computing resources. The
performance of the key components of the track reconstruction chain and its dependence on pile-up are evaluated, and
the improvement achieved compared to the previous software
version is quantified. For events with an average of 60 pp collisions per bunch crossing, the updated track reconstruction
is twice as fast as the previous version, without significant
reduction in reconstruction efficiency and while reducing the
rate of combinatorial fake tracks by more than a factor two
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at √s = 7, 8 and 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud A Abed
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo P Martinez
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen J Von
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- 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
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FL Lucio
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RY González
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
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- 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
- 01/01/2022
- Field of study
This paper presents an analysis at next-to-next-to-leading order in the theory of quantum chromodynamics for the determination of a new set of proton parton distribution functions using diverse measurements in pp collisions at \sqrt{s} = 7, 8 and 13 TeV, performed by the ATLAS experiment at the Large Hadron Collider, together with deep inelastic scattering data from ep collisions at the HERA collider. The ATLAS data sets considered are differential cross-section measurements of inclusive W^{±} and Z/gamma^{*} boson production, W^{±} and Z boson production in association with jets, t\bar{t} production, inclusive jet production and direct photon production. In the analysis, particular attention is paid to the correlation of systematic uncertainties within and between the various ATLAS data sets and to the impact of model, theoretical and parameterisation uncertainties. The resulting set of parton distribution functions is called ATLASpdf21
Corrigendum to "Search for flavour-changing neutral-current couplings between the top quark and the photon with the ATLAS detector at √s=13 TeV" (Physics Letters B, 842 (2023), 137379)
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- Zakharchuk N
- Zambito S
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeißner Sv
- Zeng Jc
- Zenger Dt
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
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- Zhang G
- Zhang J
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- Zhang L
- Zhang R
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- Zhang X
- Zhang X
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu Cg
- Zhu H
- Zhu Hl
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine Ni
- Zinsser J
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- Zormpa O
- Zou W
- Zwalinski L
- Ženiš T
- Živković L
- Publication venue
- ELSEVIER
- Publication date
- 01/01/2023
- Field of study
Performance and calibration of quark/gluon-jet taggers using 140 fb⁻¹ of 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
- 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
- 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
- Alexopoulos T
- Alfonsi F
- Algren M
- Alhroob M
- Ali B
- Ali HMJ
- Ali S
- Alibocus SW
- Aliev M
- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allen JF
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amor Dos Santos SP
- Amos KR
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Anulli F
- Aoki M
- Aoki T
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Appelt C
- Apyan A
- Aranzabal N
- Arbiol Val SJ
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Assahsah J
- Assamagan K
- Astalos R
- Atashi S
- Atkin RJ
- Atkinson M
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Auriol AD
- Austrup VA
- Avolio G
- Axiotis K
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahmani M
- Bailey AJ
- Bailey VR
- Baines JT
- Baines L
- Baker OK
- Bakos E
- Bakshi Gupta D
- Balakrishnan V
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Baltes LM
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barakat M
- Barberio EL
- Barberis D
- Barbero M
- Barel MZ
- Barends KN
- Barillari T
- Barisits M-S
- Barklow T
- Baron Moreno DA
- Baron P
- Baroncelli A
- Barone G
- Barr AJ
- Barr JD
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
- Barron U
- Barros Teixeira MG
- Barsov S
- Bartels F
- Bartoldus R
- Barton AE
- Bartos P
- Basan A
- Baselga M
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Battulga D
- Bauce M
- Bauer M
- Bauer P
- Bazzano Hurrell LT
- Beacham JB
- Beau T
- Beaucamp JY
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HP
- Becker K
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Benchekroun D
- Bendebba F
- Benhammou Y
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Beringer J
- Bernardi G
- Bernius C
- Bernlochner FU
- Bernon F
- Berrocal Guardia A
- Berry T
- Berta P
- Berthold A
- Bertram IA
- Bethke S
- Betti A
- Bevan AJ
- Bhalla NK
- Bhamjee M
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Bianco G
- Biebel O
- Bielski R
- Biglietti M
- Bindi M
- Bingul A
- Bini C
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Biros M
- Biryukov S
- Bisanz T
- Bisceglie E
- Biswal JP
- Biswas D
- Bitadze A
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Boehm B
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbély AG
- Bordulev IS
- Borecka-Bielska HM
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Bouchhar N
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bracinik J
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- Zhemchugov A
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
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- Zorbas TG
- Zormpa O
- Zou W
- 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
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
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- Acharya BS
- Achkar B
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- Addepalli SV
- Adelman J
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Search for resonant production of dark quarks in the dijet final state with the ATLAS detector
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- 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
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