191 research outputs found
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
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- Arutinov D
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- Asman B
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- Zemla A
- Zenin O
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- Zerwas D
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- Zhao Z
- Zhemchugov A
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- Zhuravlov V
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- Zimin NI
- Zimmermann R
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- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Smizanska M
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- Taiblum N
- Takahashi Y
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- Torchiani I
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- Tyrvainen H
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- Uhrmacher M
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- Varnes EW
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- Vorobel V
- Vorobiev AP
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- Vos M
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- Voss TT
- Vossebeld JH
- Vranjes N
- Vrba V
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- Vukotic I
- Wagner P
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- Wiglesworth C
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- Xie Y
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- Yagci KD
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
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- Yamanaka T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
- Yoshida R
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- Youssef S
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- Yu J
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- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
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- Zhuravlov V
- Zieminska D
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- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale 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 âs = 7TeV 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 pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy 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 jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy 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, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is 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. © 2013 CERN for the benefit of the ATLAS collaboration
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or Ï lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, Ï, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan ÎČ in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
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- Yanush S
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
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- Yoshihara K
- Young C
- Young CJ
- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zerwas D
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- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal ZâČ Models
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MS
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Gonzalez BA
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Bella LA
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
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- Armbruster AJ
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- Artamonov A
- Artoni G
- Arutinov D
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- Asman B
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- Astbury A
- Atkinson M
- Aubert B
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- Aurousseau M
- Avolio G
- Avramidou R
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
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- Backes M
- Backhaus M
- Mayes JB
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
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- Zerwas D
- della Porta GZ
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fbâ1 of sâ=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan ÎČ < 40
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Zitoun R
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- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at âs = 7 TeV with the ATLAS detector
- 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
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- 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
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- 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
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- 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
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- Atlay NB
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescua E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
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- Caforio D
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- Caminal Armadans R
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- Castillo IS
- Castillo LRF
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- Castro NF
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- Chernyatin V
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- Da Via C
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- De Pedis D
- De Regie JBDV
- de Renstrom PAB
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- Deluca C
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- Demirkoz B
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
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- Di Simone A
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- Dwuznik M
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- Ekelof T
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- El Moursli A
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- Enari Y
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- Endo M
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- Engelmann R
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- Erdmann J
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- Ereditato A
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- Eriksson D
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- Ernst M
- Ernst M
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- Errede D
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- Errede S
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- Ertel E
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- Escalier M
- Escalier M
- Esch H
- Esch H
- Escobar C
- Escobar C
- Espinal Curull X
- Espinal Curull X
- Esposito B
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- Etienne F
- Etienne F
- Etienvre AI
- Etienvre AI
- Etzion E
- Etzion E
- Evans H
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- Fabbri L
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- Facini G
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- Fakhrutdinov RM
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- Faltova J
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- Fang Y
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- Farooque T
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- Farrell S
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- Farrington SM
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- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
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- Fassouliotis D
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- Favareto A
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- Fayard L
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- Federic P
- Federic P
- Fedin OL
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- Fedorko W
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- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
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- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
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- Fenyuk AB
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- Fernando W
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- Ferrag S
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- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
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- Ferrari A
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- Ferrari P
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- Ferretti C
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- Fiascaris M
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- Fiedler F
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- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
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- Fincke-Keeler M
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- Fiolhais MCN
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- Fiorini L
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- Firan A
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- Fitzgerald EA
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- Fleck I
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- Fleischmann P
- Fleischmann P
- Fleischmann S
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- Fletcher G
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- Fletcher GT
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- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
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- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
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- Fournier D
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- Francavilla P
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- Francis D
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- Franklin M
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- Franz S
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- French ST
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- Friedrich C
- Friedrich F
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- Fulsom BG
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- Gabizon O
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- Gabrielli A
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- Gadatsch S
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- Gadomski S
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- Gagliardi G
- Gagliardi G
- Gagnon P
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- Galea C
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- Galhardo B
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- Gallas EJ
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- Gallo V
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- Gallop BJ
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- Gallus P
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- Gandrajula RP
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- Gao J
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- Gaob J
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- Garcia BRM
- Garcia C
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- Gardner RW
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- Garelli N
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- Garonne V
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- Garrido MDMC
- Gatti C
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- Gaudio G
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- Gaur B
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- Gauzzi P
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- Gavrilenko IL
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- Gay C
- Gay C
- Gaycken G
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- Gazis EN
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- Ge P
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- Gecse Z
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- Gee CNP
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- Geerts DAA
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- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
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- Gemme C
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- Gemmell A
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- Genest MH
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- Gentile S
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- George M
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- George S
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- Gerbaudo D
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- Gershon A
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- Ghazlane H
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- Ghodbane N
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- Giacobbe B
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- Giagu S
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- Giangiobbe V
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- Giannetti P
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- Gillam TPS
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- Gillberg D
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- Gillman AR
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- Gingrich DM
- Gingrich M
- Giokaris N
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- Giordani MP
- Giordani MP
- Giordano R
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- Giorgi FM
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- Giraud PF
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- Giugni D
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- Giuliani C
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- Giunta M
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- Gjelsten BK
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- Gkialas I
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- Gladilin LK
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- Gorbounov PA
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- Gordon HA
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- Gorelov I
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- Gorini B
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- Gorini E
- Gorini E
- Gorisek A
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- Gornicki E
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- Goshaw AT
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- Gostkin MI
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- Grabas HMX
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of âs = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentreâofâmassframeisusedtosuppressthelargemultiâjetbackground.ThecrossâsectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Long-range and short-range dihadron angular correlations in central PbPb collisions at âsNN=2.76 TeV
- Author
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- Mekterovic D
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- Melzer-Pellmann IA
- Menasce D
- Mendez H
- Meneghelli M
- Meneguzzo AT
- Menendez JF
- Menendez JF
- Meng X
- Menichelli M
- Mercadante PG
- Mercier D
- Meridiani P
- Meridiani P
- Merino G
- Merino G
- Merkel P
- Merlo JP
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- Merola M
- Merschmeyer M
- Mersi S
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- Merz J
- Mesa D
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- Meschi E
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- Messineo A
- Mestvirishvili A
- Mestvirishvili A
- Metson S
- Metson S
- Meyer A
- Meyer AB
- Miao T
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- Miceli T
- Miceli T
- Migliore E
- Mignerey AC
- Mikami Y
- Mikulec I
- Mila G
- Milenovic P
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- Militaru O
- Miller DH
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- Moeller A
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- Mohammadi A
- Mohanty AK
- Mohanty GB
- Mohapatra A
- Mohr N
- Moisenz P
- Moisenz P
- Molnar J
- Monaco V
- Mondal NK
- Montalvo R
- Montanari A
- Montanino D
- Montanino D
- Montoya CAC
- Moon DH
- Moon DH
- Mooney M
- Moortgat F
- Moortgat F
- Moreno BG
- Moreno SC
- Moreno SC
- Moroni L
- Morovic S
- Morse DM
- Moser R
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- Mossolov V
- Mott A
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- Mousa J
- Mozer MU
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- Mrenna S
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- Mucibello L
- Mueller S
- Mulders M
- Mulders M
- Muller T
- Mundim L
- Muniz L
- Muniz L
- Muntel M
- Mura B
- Murray M
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- Musenich R
- Musich M
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- My S
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- Najafabadi MM
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- Naumann-Emme S
- Navarria FL
- Nawrocki K
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- Nayak A
- Nayak A
- Nef P
- Nef R
- Nespolo M
- Nessi-Tedaldi F
- Nessi-Tedaldi F
- Nesvold E
- Nesvold E
- Neu C
- Neumeister N
- Newbold DM
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- Newman HB
- Newman HB
- Newman-Holmes C
- Newman-Holmes C
- Newsom CR
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- Nguyen D
- Nguyen D
- Nguyen H
- Nguyen H
- Nguyen M
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- Nicolaou C
- Niegel M
- Nikitenko A
- Nikitenko A
- Nikolic M
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- Nirunpong K
- Nirunpong K
- Nishu N
- Nogima H
- Noonan D
- Norbeck E
- Norbeck E
- Nourbakhsh S
- Novaes SF
- Nowack A
- Nowak F
- Ntomari E
- Nuzzo S
- O'Brien C
- O'Brien C
- O'Dell V
- O'Dell V
- Oberst O
- Obertino MM
- Obraztsov S
- Obraztsov S
- Ocalan K
- Ocalan K
- Ochando C
- Ochesanu S
- Odell N
- Odorici F
- Oehler A
- Oguri V
- Olaiya E
- Olaiya E
- Oliveros AFO
- Oliveros S
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- Olson J
- Olson J
- Olzem J
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- Onel Y
- Onen JHA
- Onengut G
- Onengut G
- Onig SK
- Orbaker D
- Oreshkin V
- Oreshkin V
- Organtini G
- Orimoto T
- Orimoto T
- Orsini L
- Orsini L
- Osipenkov I
- Ostapchuk A
- Otiougova P
- Otiougova P
- Ott J
- Ovyn S
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- Ozdemir K
- Ozkorucuklu S
- Ozkorucuklu S
- Ozok F
- Ozok F
- Ozpineci A
- Ozpineci A
- Ozturk S
- Ozturk S
- Pacifico N
- Padhi S
- Padhi S
- Padley BP
- Padula SS
- Paganini P
- Pagano D
- Paganoni M
- Pakhotin Y
- Pakhotin Y
- Palichik V
- Palichik V
- Palinkas J
- Palla F
- Palmer C
- Palmer C
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- Panagiotou A
- Pandolfi F
- Pant LM
- Panwalkar S
- Paoletti S
- Paolucci P
- Papacz P
- Papadopoulos I
- Papageorgiou A
- Papageorgiou A
- Pape L
- Pape L
- Paramatti R
- Parashar N
- Pardo PL
- Pardo PL
- Pardos CD
- Pardos CD
- Park C
- Park C
- Park H
- Park H
- Park IC
- Park IC
- Park S
- Park S
- Park SK
- Park SK
- Parracho PGF
- Parracho PGF
- Pashenkov A
- Pashenkov A
- Passaseo M
- Pastrone N
- Patel R
- Patras V
- Patterson JR
- Patterson JR
- Paulini M
- Paulini M
- Paus C
- Pauss F
- Pauss F
- Pavlov B
- Pavlunin V
- Pavlunin V
- Pearson T
- Pedrini D
- Pegna DL
- Peiffer T
- Pelayo JP
- Pellett D
- Pellett D
- Pelliccioni M
- Pelliccioni M
- Pens AD
- Penzo A
- Penzo A
- Perchalla L
- Pereira AV
- Pereira AV
- Perelygin V
- Perelygin V
- Perera L
- Perez E
- Perez E
- Perez JAC
- Perez JAC
- Perfilov M
- Perieanu A
- Peris AD
- Pernicka M
- Perries S
- Perrotta A
- Perrozzi L
- Pesaresi M
- Pesaresi M
- Petkov P
- Petrakou E
- Petridis K
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- Petrilli A
- Petrilli A
- Petrillo G
- Petrov P
- Petrov P
- Petrov V
- Petrov V
- Petrucciani G
- Petrucciani G
- Petrushanko S
- Petyt D
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- Pfeiffer A
- Pfeiffer A
- Pi H
- Pi H
- Piccolo D
- Pieri M
- Pieri M
- Pierini M
- Pierini M
- Pierro GA
- Pieta H
- Pietsch N
- Pimia M
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- Pin A
- Pineda AM
- Pineda AM
- Pioppi M
- Pioppi M
- Piotrzkowski K
- Piparo D
- Piperov S
- Piroue P
- Pitzl D
- Pivarski J
- Plager C
- Plager C
- Plestina R
- Pol ME
- Polatoz A
- Polatoz A
- Polese G
- Polese G
- Polic D
- Poll A
- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popov V
- Popov V
- Pordes R
- Pordes R
- Pozdnyakov A
- Pozzobon N
- Prescott C
- Prescott C
- Primavera F
- Prokofyev O
- Prokofyev O
- Prosper H
- Prosper H
- Ptochos F
- Puerta J
- Pugliese G
- Puigh D
- Puigh D
- Puljak I
- Punz T
- Punz T
- Qazi S
- Qazi S
- Qian SJ
- Quan X
- Quast G
- Quertenmont L
- Quertenmont L
- Rabbertz K
- Racz A
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- Radburn-Smith BC
- Radburn-Smith BC
- Ragazzi S
- Rahatlou S
- Rahmat R
- Raics P
- Raidal M
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- Ralph D
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- Ranieri R
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- Ranjan K
- Rappoccio S
- Raspereza A
- Ratnikov F
- Ratnikova N
- Ratti SP
- Raupach F
- Raval A
- Ray EAF
- Raymond DM
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- Razis PA
- Rebane L
- Rebassoo F
- Rebassoo F
- Redaelli N
- Redjimi R
- Redondo I
- Reeder D
- Regenfus C
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- Reithler H
- Rekovic V
- Remington R
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- Rios AAO
- Rivero CM
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- Rizzi A
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- Ro SR
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- Roberts J
- Robles J
- Robles J
- Robmann P
- Robmann P
- Rodenburg M
- Rodozov M
- Rodrigo T
- Rodrigo T
- Rodriguez JL
- Rodriguez JL
- Rodriguez-Marrero AY
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- Rogerson S
- Roh Y
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- Rohringer H
- Roland B
- Roland C
- Roland G
- Rolandi G
- Rolandi G
- Romano F
- Romanowska-Rybinska K
- Romanowska-Rybinska K
- Romeo F
- Romero A
- Romero A
- Romero L
- Romero L
- Rommerskirchen T
- Rommerskirchen T
- Rompotis N
- Rompotis N
- Ronchese P
- Ronga FJ
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- Rose A
- Rose A
- Rose K
- Roselli G
- Rosin M
- Rosowsky A
- Ross I
- Rossato K
- Rossi AM
- Rossin R
- Rossin R
- Rossini M
- Rossini M
- Rougny R
- Rovelli C
- Rovelli C
- Rovelli T
- Rovere M
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- Ruchti R
- Rudolph M
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- Rumerio P
- Rusack R
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- Ryd A
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- Ryu G
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- Ryutin R
- Ryutin R
- Sabes D
- Sabonis T
- Sabonis T
- Sacchi R
- Sacchi R
- Safarzadeh B
- Safonov A
- Safronov G
- Safronov G
- Saha A
- Saini LK
- Saka H
- Sakharov A
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- Sala S
- Salerno R
- Salur S
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- Salvati E
- Sammet J
- Sanabria JC
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- Sanchez-Hernandez A
- Sander C
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- Sanders S
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- Santaolalla J
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- Santocchia A
- Santoro A
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- Saout C
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- Schieferdecker P
- Schilling FP
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- Schnetzer S
- Schoerner-Sadenius T
- Schofbeck R
- Schott G
- Schroder M
- Schul N
- Schum T
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- Selvaggi M
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- Sen N
- Sen S
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- Sengupta S
- Senkin S
- Senkin S
- Seo E
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- Seo H
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- Serban AT
- Serin M
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- Sexton-Kennedy E
- Sexton-Kennedy E
- Sguazzoni G
- Sharma A
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- Sharma A
- Sharma S
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- Sharma V
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- Sharp P
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- Sheldon P
- Shen BC
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- Shepherd-Themistocleous CH
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- Shi X
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- Shin K
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- Shipsey I
- Shiu JG
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- Shmatov S
- Shmatov S
- Shrestha S
- Shreyber I
- Shukla P
- Shumeiko N
- Sibille J
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- Vila I
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- Villasenor-Cendejas LM
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Vinogradov A
- Virdee T
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- Vitulo P
- Viviani C
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- Volkov A
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- Volobouev I
- Volodko A
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- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu I
- Yu SS
- Yu SS
- Yumiceva F
- Yumiceva F
- Yun JC
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zakaria M
- Zalewski P
- Zalewski R
- Zanetti M
- Zang J
- Zang SL
- Zang SL
- Zarubin A
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeuner WD
- Zeyrek M
- Zeyrek M
- Zhang J
- Zhang L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhokin A
- Zhu B
- Zhu RY
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zou W
- Zuranski A
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article, which can be accessed from the link below.First measurements of dihadron correlations for charged particles are presented
for central PbPb collisions at a nucleon-nucleon center-of-mass energy of 2.76TeV over a broad range in relative pseudorapidity ( ) and the full range of relative azimuthal angle ( ). The data were collected with the CMS detector, at the LHC. A broadening of the away-side ( ) azimuthal correlation is observed at all , as compared to the measurements in pp collisions. Furthermore, long-range dihadron correlations in are observed for particles with similar values. This phenomenon, also known as the \ridge",
persists up to at least j j = 4. For particles with transverse momenta (pT) of 2-4 GeV/c, the ridge is found to be most prominent when these particles are correlated with particles of pT = 2-6 GeV/c, and to be much reduced when paired with particles of pT = 10-12 GeV/c
Measurement of the cross-section for b-jets produced in association with a Z boson at root s=7 TeV with the ATLAS detector ATLAS Collaboration
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Ziolkowski M
- Zitoun R
- Zivkovic L
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- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
A measurement is presented of the inclusive cross-section for b-jet production in association with a Z boson in pp collisions at a centre-of-mass energy of root s = 7 TeV. The analysis uses the data sample collected by the ATLAS experiment in 2010, corresponding to an integrated luminosity of approximately 36 pb(-1). The event selection requires a Z boson decaying into high P-T electrons or muons, and at least one b-jet, identified by its displaced vertex, with transverse momentum p(T) > 25 GeV and rapidity vertical bar y vertical bar < 2.1. After subtraction of background processes, the yield is extracted from the vertex mass distribution of the candidate b-jets. The ratio of this cross-section to the inclusive Z cross-section (the average number of b-jets per Z event) is also measured. Both results are found to be in good agreement with perturbative QCD predictions at next-to-leading order
Flavor tagged time-dependent angular analysis of the B0s â J/ÏÏ decay and extraction of ÎÎs and the weak phase Ïs in ATLAS
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
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- Zhemchugov A
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- Zieminska D
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- Zimmermann R
- Zimmermann S
- Zimmermann S
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- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the B0sâJ/ÏÏ decay parameters, updated to include flavor tagging is reported using 4.9ââfbâÂč of integrated luminosity collected by the ATLAS detector from âs=7ââTeV pp collisions recorded in 2011 at the LHC. The values measured for the physical parameters are
Ïs=0.12±0.25(stat)±0.05(syst)âârad
ÎÎs=0.053±0.021(stat)±0.010(syst)ââpsâÂč
Îs=0.677±0.007(stat)±0.004(syst)ââpsâÂč
|Aâ„(0)|2=0.220±0.008(stat)±0.009(syst)
|A0(0)|2=0.529±0.006(stat)±0.012(syst)
ÎŽâ„=3.89±0.47(stat)±0.11(syst)âârad
where the parameter ÎÎs is constrained to be positive. The S-wave contribution was measured and found to be compatible with zero. Results for Ïs and ÎÎs are also presented as 68% and 95% likelihood contours, which show agreement with the Standard Model expectations
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