15 research outputs found
Measurement of the top-quark mass in the fully hadronic decay channel from ATLAS data at s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyka L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
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- Allport PP
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- Argyropoulos S
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- Armbruster AJ
- Arnaez O
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- Arratia M
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- Artamonov A
- Artoni G
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- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2014
- Field of study
The mass of the top quark is measured in a data set corresponding to 4.6 fb−1 of proton--proton collisions with centre-of-mass energy s=7 TeV collected by the ATLAS detector at the LHC. Events consistent with hadronic decays of top--antitop quark pairs with at least six jets in the final state are selected. The substantial background from multijet production is modelled with data-driven methods that utilise the number of identified b-quark jets and the transverse momentum of the sixth leading jet, which have minimal correlation. The top-quark mass is obtained from template fits to the ratio of three-jet to dijet mass. The three-jet mass is calculated from the three jets of a top-quark decay. Using these three jets the dijet mass is obtained from the two jets of the W boson decay. The top-quark mass obtained from this fit is thus less sensitive to the uncertainty in the energy measurement of the jets. A binned likelihood fit yields a top-quark mass of mt = 175.1 ± 1.4 (stat.) ± 1.2 (syst.) GeV.publishedVersio
Performance of algorithms that reconstruct missing transverse momentum in √s= 8 TeV proton-proton collisions in the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
The reconstruction and calibration algorithms used to calculate missing transverse momentum (EmissT ) with the ATLAS detector exploit energy deposits in the calorimeter and tracks reconstructed in the inner detector as well as the muon spectrometer. Various strategies are used to suppress effects arising from additional proton–proton interactions, called pileup, concurrent with the hard-scatter processes. Tracking information is used to distinguish contributions from the pileup interactions using their vertex separation along the beam axis. The performance of the EmissT reconstruction algorithms, especially with respect to the amount of pileup, is evaluated using data collected in proton–proton collisions at a centre-of-mass energy of 8 TeV during 2012, and results are shown for a data sample corresponding to an integrated luminosity of 20.3fb−1. The simulation and modelling of EmissT in events containing a Z boson decaying to two charged leptons (electrons or muons) or a W boson decaying to a charged lepton and a neutrino are compared to data. The acceptance for different event topologies, with and without high transverse momentum neutrinos, is shown for a range of threshold criteria for EmissT , and estimates of the systematic uncertainties in the EmissT measurements are presented.ATLAS Collaboration, for complete list of authors see dx.doi.org/10.1140/epjc/s10052-017-4780-2Funding: We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently.We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF and DNSRC, Denmark; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, HGF, and MPG, Germany; GSRT, Greece; RGC, Hong Kong SAR, China; ISF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; RCN, Norway; MNiSW and NCN, Poland; FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, UK; DOE and NSF, United States of America. In addition, individual groups and members have received support from BCKDF, the Canada Council, CANARIE, CRC, Compute Canada, FQRNT, and the Ontario Innovation Trust, Canada; EPLANET, ERC, FP7, Horizon 2020 and Marie Skłodowska-Curie Actions, European Union; Investissements d’Avenir Labex and Idex, ANR, Région Auvergne and Fondation Partager le Savoir, France; DFG and AvH Foundation, Germany; Herakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF; BSF, GIF and Minerva, Israel; BRF, Norway; Generalitat de Catalunya, Generalitat Valenciana, Spain; the Royal Society and Leverhulme Trust, United Kingdom. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN, the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA), the Tier-2 facilities worldwide and large non-WLCG resource providers. Major contributors of computing resources are listed in Ref. [58].</p
Charged-particle distributions in pp interactions at √s = 8 TeV measured with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- Abolins M
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyka L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
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- Alpigiani C
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
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- Amundsen G
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- Angelidakis S
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- Armadans RC
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- van Woerden MC
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- Vandelli W
- Vanguri R
- Vaniachine A
- Vankov P
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasquez JG
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Verzini MJA
- Vest A
- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Vigne R
- Villa M
- Villara DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vittori C
- Vivarelli I
- Vlachos S
- Vlasak M
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Walls FMG
- Wang C
- Wang C
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang K
- Wang R
- Wang SM
- Wang T
- Wang T
- Wang X
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Washbrook A
- Watkins PM
- Watson AT
- Watson IJ
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Webb S
- Weber MS
- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weiser C
- Weits H
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Wessels M
- Wetter J
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White MJ
- White R
- White S
- Whiteson D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wu M
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang Y
- Yang Z
- Yange H
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yuen SPY
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/07/2016
- Field of study
This paper presents measurements of distributions
of charged particles which are produced in proton–
proton collisions at a centre-of-mass energy of √s = 8 TeV
and recorded by the ATLAS detector at the LHC. A special
dataset recorded in 2012 with a small number of interactions
per beam crossing (below 0.004) and corresponding to an
integrated luminosity of 160 µb−1 was used. A minimumbias
trigger was utilised to select a data sample of more than
9 million collision events. The multiplicity, pseudorapidity,
and transverse momentum distributions of charged particles
are shown in different regions of kinematics and chargedparticle
multiplicity, including measurements of final states at
high multiplicity. The results are corrected for detector effects
and are compared to the predictions of various Monte Carlo
event generator models which simulate the full hadronic final
state
Standalone vertex finding in the ATLAS muon spectrometer
- Author
- Publication venue
- Publication date
- 01/01/2016
- Field of study
Standalone vertex finding in the ATLAS muon spectrometer
- Author
- Aad G.
- Abajyan T.
- Abbott B.
- Abdallah J.
- Abdinov O.
- Aben R.
- Abi B.
- Abolins M.
- AbouZeid O. S.
- Abramowicz H.
- Abreu H.
- Abulaitia Y.
- Acharya B. S.
- Adamczyka L.
- Adams D. L.
- Addy T. N.
- Adelman J.
- Adomeit S.
- Adye T.
- Aefsky S.
- Agatonovic-Jovinb T.
- Aguilar-Saavedra J. A.
- Agustoni M.
- Ahlen S. P.
- Ahmad A.
- Ahmadov F.
- Aielli G.
- Akesson T. P. A.
- Akimoto G.
- Khalek S. A.
- Krasznahorkay Attila
- Nagai Yoshikazu
- Pásztor Gabriella
- Tóth József
- Publication venue
- Publication date
- 01/01/2014
- Field of study
A dedicated reconstruction algorithm to find decay vertices in the ATLAS muon spectrometer is presented. The algorithm searches the region just upstream of or inside the muon spectrometer volume for multi-particle vertices that originate from the decay of particles with long decay paths. The performance of the algorithm is evaluated using both a sample of simulated Higgs boson events, in which the Higgs boson decays to long-lived neutral particles that in turn decay to bb final states, and pp collision data at √ s = 7 TeV collected with the ATLAS detector at the LHC during 2011
A neural network clustering algorithm for the ATLAS silicon pixel detector
- Author
- Aad G.
- Abbott B.
- Abdallah J.
- Abdinov O.
- Aben R.
- Abi B.
- Abolins M.
- AbouZeid O. S.
- Abramowicz H.
- Abreu H.
- Abreu R.
- Abulaitia Y.
- Acharya B. S.
- Adamczyka L.
- Adams D. L.
- Adelman J.
- Adomeit S.
- Adye T.
- Agatonovic-Jovin T.
- Aguilar-Saavedra J. A.
- Agustoni M.
- Ahlen S. P.
- Ahmadov F.
- Aielli G.
- Akerstedt H.
- Akesson T. P. A.
- Akimoto G.
- Akimov A. V.
- Alberghi G. L.
- Khalek S. A.
- Krasznahorkay Attila
- Nagai Yoshikazu
- Pásztor Gabriella
- Tóth József
- Publication venue
- Publication date
- 01/01/2014
- Field of study
A novel technique to identify and split clusters created by multiple charged particles in the AT- LAS pixel detector using a set of artificial neural networks is presented. Such merged clusters are a common feature of tracks originating from highly energetic objects, such as jets. Neural networks are trained using Monte Carlo samples produced with a detailed detector simulation. This technique replaces the former clustering approach based on a connected component analysis and charge in- terpolation. The performance of the neural network splitting technique is quantified using data from proton–proton collisions at the LHC collected by the ATLAS detector in 2011 and from Monte Carlo simulations. This technique reduces the number of clusters shared between tracks in highly energetic jets by up to a factor of three. It also provides more precise position and error estimates of the clusters in both the transverse and longitudinal impact parameter resolution
Recommended from our members
Standalone vertex finding in the ATLAS muon spectrometer
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyka L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Aefsky S
- Agatonovic-Jovinb T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmad A
- Ahmadov F
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimontia G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjosa N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik E
- Bella L Aperio
- Coutinho Y Amaral
- Dos Santos SP Amor
- Gonzalez B Alvarez
- Khalek S Abdel
- Verzini MJ Alconada
- Publication venue
- eScholarship, University of California
- Publication date
- 01/02/2014
- Field of study
A dedicated reconstruction algorithm to find decay vertices in the ATLAS muon spectrometer is presented. The algorithm searches the region just upstream of or inside the muon spectrometer volume for multi-particle vertices that originate from the decay of particles with long decay paths. The performance of the algorithm is evaluated using both a sample of simulated Higgs boson events, in which the Higgs boson decays to long-lived neutral particles that in turn decay to bb final states, and pp collision data at √s = 7 TeV collected with the ATLAS detector at the LHC during 2011
Recommended from our members
Search for metastable heavy charged particles with large ionisation energy loss in pp collisions at vs root s=8 TeV using the ATLAS experiment
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharyaa BS
- Adamczyka L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Bella L Aperio
- Coutinho Y Amaral
- Dos Santos SP Amor
- Gonzalez B Alvarez
- Piqueras D Alvarez
- Verzini MJ Alconada
- Publication venue
- eScholarship, University of California
- Publication date
- 03/09/2015
- Field of study
Recommended from our members
A neural network clustering algorithm for the ATLAS silicon pixel detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyka L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Araquea JP
- Arce ATH
- Arguin JF
- Argyropoulos S
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Bella LA
- Coutinho YA
- Gonzalez BA
- Khalek SA
- Verzini MJA
- Åkesson TPA
- Publication venue
- eScholarship, University of California
- Publication date
- 01/09/2014
- Field of study
A novel technique to identify and split clusters created by multiple charged particles in the ATLAS pixel detector using a set of artificial neural networks is presented. Such merged clusters are a common feature of tracks originating from highly energetic objects, such as jets. Neural networks are trained using Monte Carlo samples produced with a detailed detector simulation. This technique replaces the former clustering approach based on a connected component analysis and charge interpolation. The performance of the neural network splitting technique is quantified using data from proton-proton collisions at the LHC collected by the ATLAS detector in 2011 and from Monte Carlo simulations. This technique reduces the number of clusters shared between tracks in highly energetic jets by up to a factor of three. It also provides more precise position and error estimates of the clusters in both the transverse and longitudinal impact parameter resolution
Constraints on off-shell Higgs boson production and the Higgs boson total width in ZZ -> 4l and ZZ -> 2l2v final states with the ATLAS detector
- Author
- Aaboudd M.
- Aad G.
- Abbott B.
- Abdinov O.
- Abeloos B.
- Abhayasinghe D. K.
- Abidi S. H.
- AbouZeid O. S.
- Abraham N. L.
- Abramowicz H.
- Abreu H.
- Abulaiti Y.
- Acharyaa B. S.
- Adachi S.
- Adam L.
- Adamczyka L.
- Adelman J.
- Adersberger M.
- Adiguzel Aytül
- Adye T.
- Affolder A. A.
- Afik Y.
- Agheorghiesei C.
- Aguilar-Saavedra J. A.
- Ahmadov F.
- Aielli G.
- Akatsuka S.
- Akesson T. P. A.
- Akilli E.
- Akimov A. V.
- Alberghi G. L.
- Alberich L. Cerda
- Albert J.
- Albicocco P.
- Alderweireldt S.
- Aleksa M.
- Aleksandrov I. N.
- Alexa C.
- Alexopoulos T.
- Alhroob M.
- Ali B.
- Alimonti G.
- Alison J.
- Alkire S. P.
- Allaire C.
- Allbrooke B. M. M.
- Allen B. W.
- Allport P. P.
- Aloisio A.
- Alonso A.
- Alonso F.
- Alpigiani C.
- Alshehri A. A.
- Alstaty M. I.
- Alvarez Piqueras D.
- Alviggi M. G.
- Amadio B. T.
- Ambler A.
- Ambroz L.
- Amelung C.
- Amidei D.
- Amoroso S.
- Amrouche C. S.
- Anastopoulos C.
- Ancu L. S.
- Andari N.
- Andeen T.
- Anders C. F.
- Anders J. K.
- Anderson K. J.
- Andreazza A.
- Andrei V.
- Anelli C. R.
- Angelidakis S.
- Angelozzi I.
- Angerami A.
- Anisenkov A. V.
- Annovi A.
- Antel C.
- Anthony M. T.
- Antonelli M.
- Antrim D. J. A.
- Anulli F.
- Aoki M.
- Aparisi Pozo J. A.
- Arabidze G.
- Aranda C. Padilla
- Araque J. P.
- Araya S. Tapia
- Arce A. T. H.
- Ardell R. E.
- Arduh F. A.
- Arguin J-F.
- Argyropoulos S.
- Armadans R. Caminal
- Armbruster A. J.
- Armitage L. J.
- Armstrong A.
- Arnaez O.
- Arnold H.
- Arratia M.
- Arslan O.
- Artamonov A.
- Artoni G.
- Artz S.
- Asai S.
- Asbah N.
- Asimakopoulou E. M.
- Asquith L.
- Assamagan K.
- Astalos R.
- Astigarraga M. E. Pozo
- Atkin R. J.
- Atkinson M.
- Atlay N. B.
- Augsten K.
- Avolio G.
- Avramidou R.
- Ayoub M. K.
- Azuelos G.
- Baas A. E.
- Baca M. J.
- Bachacou H.
- Bachas K.
- Backes M.
- Bagnaia P.
- Bahilo J. J. Lozano
- Bahmani M.
- Bahrasemani H.
- Bailey A. J.
- Baines J. T.
- Bajic M.
- Bakalis C.
- Baker O. K.
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- Bandyopadhyay A.
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- Baroncelli A.
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- Barton A. E.
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- Bates R. L.
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- Bellagamba L.
- Bellerive A.
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- Bellos P.
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- Belyaev N. L.
- Benary O.
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- Blazek T.
- Bloch I.
- Blocker C.
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- Blumenschein U.
- Blunier Dr.
- Bobbink G. J.
- Bobrovnikov V. S.
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- Boeriu O. E. Vickey
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- Publication venue
- 'Elsevier BV'
- Publication date
- 03/03/2021
- Field of study
A measurement of off-shell Higgs boson production in the ZZ -> 4l and ZZ -> 2l2v decay channels, where stands for either an electron or a muon, is performed using data from proton-proton collisions at a centre-of-mass energy of root s = 13 TeV. The data were collected by the ATLAS experiment in 2015 and 2016 at the Large Hadron Collider, and they correspond to an integrated luminosity of 36.1 fb(-1). An observed (expected) upper limit on the off-shell Higgs signal strength, defined as the event yield normalised to the Standard Model prediction, of 3.8 (3.4) is obtained at 95% confidence level (CL). Assuming the ratio of the Higgs boson couplings to the Standard Model predictions is independent of the momentum transfer of the Higgs production mechanism considered in the analysis, a combination with the on-shell signal-strength measurements yields an observed (expected) 95% CL upper limit on the Higgs boson total width of 14.4 (15.2) MeV. (C) 2018 The Author. Published by Elsevier B.V