3 research outputs found
Performance of the ATLAS track reconstruction algorithms in dense environments in LHC Run 2
- Author
- Aaboudd M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaitia Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TP
- Akimov AV
- Alberghia GL
- Alberich LC
- Albert J
- Albicocco P
- Aleksa M
- Aleksandrov IN
- Alexab C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimontia G
- Alison J
- Alkire SP
- Allbrooke BMM
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- Aloisioa A
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- Amundsen G
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- Andari N
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- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkovc AV
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- Annovia A
- Antela C
- Antonelli M
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- Antrim DJ
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- Aoki M
- Arabidze G
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- Argyropoulos S
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- Armadans RC
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- Armitage LJ
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- Artamonov A
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- Walls FMG
- Yildiz HD
- Publication venue
- Publication date
- 01/01/2017
- Field of study
With the increase in energy of the Large Hadron Collider to a centre-of-mass energy of 13 TeV for Run 2, events with dense environments, such as in the cores of highenergy jets, became a focus for new physics searches as well as measurements of the Standard Model. These environments are characterized by charged-particle separations of the order of the tracking detectors sensor granularity. Basic track quantities are compared between 3.2 fb(-1) of data collected by the ATLAS experiment and simulation of protonproton collisions producing high-transverse-momentum jets at a centre-of-mass energy of 13 TeV. The impact of chargedparticle separations and multiplicities on the track reconstruction performance is discussed. The track reconstruction efficiency in the cores of jets with transverse momenta between 200 and 1600 GeV is quantified using a novel, datadriven, method. The method uses the energy loss, dE/ dx, to identify pixel clusters originating from two charged particles. Of the charged particles creating these clusters, themeasured fraction that fail to be reconstructed is 0.061 +/- 0.006 (stat.) +/- 0.014 (syst.) and 0.093 +/- 0.017 (stat.) +/- 0.021 (syst.) for jet transverse momenta of 200-400GeV and 1400-1600GeV, respectively
Measurement of W(+/-)Z production in proton-proton collisions at root s=7 TeV with the ATLAS detector
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- Zajacova Z
- Zanelloa L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenisa T
- Zenz S
- Zerwas D
- Zhand Z
- Zhang H
- Zhang J
- Zhang Z
- Zhangb D
- Zhangd X
- Zhao L
- Zhao T
- Zhaob Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu H
- Zhu J
- Zhuang X
- Zhub Y
- Zhud CG
- Zhuravlov V
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonosa Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccolia A
- Zutshi V
- Zwalinski L.
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
A study of W(+/-)Z production in proton-proton collisions at root s = 7 TeV is presented using data corresponding to an integrated luminosity of 4.6 fb(-1) collected with the ATLAS detector at the Large Hadron Collider in 2011. In total, 317 candidates, with a background expectation of 68 +/- 10 events, are observed in double-leptonic decay final states with electrons, muons and missing transverse momentum. The total cross-section is determined to be sigma(tot)(WZ) = 19.0(-1.3)(+1.4)(stat.) +/- 0.9(syst.) +/- 0.4(lumi.) pb, consistent with the Standard Model expectation of 17.6(-1.0)(+1.1) pb. Limits on anomalous triple gauge boson couplings are derived using the transverse momentum spectrum of Z bosons in the selected events. The cross-section is also presented as a function of Z boson transverse momentum and diboson invariant mass
Jet energy measurement with the ATLAS detector in proton-proton collisions at sqrt(s)=7 TeV
- Author
- Aa FP
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Publication venue
- Publication date
- 01/01/9999
- Field of study
The jet energy scale (JES) and its systematic uncertainty are determined for jets measured with the ATLAS
detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7 TeV corresponding to an
integrated luminosity of 38 pb−1. Jets are reconstructed with the anti-kt algorithm with distance parameters R = 0.4 or
R = 0.6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse
momenta pT ≥ 20 GeV and pseudorapidities |h| < 4.5. The JES systematic uncertainty is estimated using the single
isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between
central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations.
The JES uncertainty is less than 2.5% in the central calorimeter region (|h| < 0.8) for jets with 60 ≤ pT < 800 GeV,
and is maximally 14% for pT < 30 GeV in the most forward region 3.2 ≤ |h| < 4.5. The uncertainty for additional
energy from multiple proton-proton collisions in the same bunch crossing is less than 1.5% per additional collision
for jets with pT > 50 GeV after a dedicated correction for this effect. The JES is validated for jet transverse momenta
up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such
as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT
jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell
energy density weighting or hadronic properties of jets, providing an improved jet energy resolution and a reduced
flavour dependence of the jet response. The JES systematic uncertainty determined from a combination of in situ
techniques are consistent with the one derived from single hadron response measurements over a wide kinematic range.
The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special
cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating
from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined