413 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
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- Achkar B
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fbâ1 of â s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Zarzhitsky P
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- Zhemchugov A
- Zheng S
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- Zitoun R
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- 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
Cancer Biomarker Discovery: The Entropic Hallmark
- Author
- A Alcaraz
- A Arabzadeh
- A Bagri
- A Balbin
- A Bantis
- A Ben-Naim
- A Bolander
- A Buhmeida
- A Burykin
- A Chetcuti
- A de Baey
- A Efeyan
- A Eroglu
- A Fabarius
- A Forget
- A Fujita
- A Geirsson
- A Geirsson
- A Geirsson
- A Guffanti
- A Hugel
- A Inoue
- A Isidoro
- A Jang
- A Kollara
- A Kuzmanov
- A Lundqvist
- A Maria McCrohan
- A Marreiros
- A Mendes
- A Mitra
- A Nassar
- A Petitjean
- A Petitjean
- A Pinzon-Charry
- A Richmond
- A Roesch
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- William C. S. Cho
- WK Kaufmann
- WK Lee
- X Chen
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- X Dong
- X Huang
- X Li
- X Liu
- X Liu
- X Meng
- X Ouyang
- X Tang
- X Wu
- X Zhang
- XJ Yang
- XQ Wang
- Y Bu
- Y Cai
- Y Deng
- Y Ito
- Y Katagiri
- Y Kozuka
- Y Lai
- Y Liu
- Y Lu
- Y Lu
- Y Ohyama
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- Y Yang
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- YB Lim
- YC Chao
- YJ Ko
- YL Liu
- YN Liu
- YT Sasaki
- YT Sasaki
- YU Katagiri
- Z Jiang
- Z Jiang
- Z Jiang
- Z Jiang
- Z Jiang
- Z Rudzki
- ZA Dotan
- ZR Yurkovetsky
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Background: It is a commonly accepted belief that cancer cells modify their transcriptional state during the progression of the disease. We propose that the progression of cancer cells towards malignant phenotypes can be efficiently tracked using high-throughput technologies that follow the gradual changes observed in the gene expression profiles by employing Shannon's mathematical theory of communication. Methods based on Information Theory can then quantify the divergence of cancer cells' transcriptional profiles from those of normally appearing cells of the originating tissues. The relevance of the proposed methods can be evaluated using microarray datasets available in the public domain but the method is in principle applicable to other high-throughput methods. Methodology/Principal Findings: Using melanoma and prostate cancer datasets we illustrate how it is possible to employ Shannon Entropy and the Jensen-Shannon divergence to trace the transcriptional changes progression of the disease. We establish how the variations of these two measures correlate with established biomarkers of cancer progression. The Information Theory measures allow us to identify novel biomarkers for both progressive and relatively more sudden transcriptional changes leading to malignant phenotypes. At the same time, the methodology was able to validate a large number of genes and processes that seem to be implicated in the progression of melanoma and prostate cancer. Conclusions/Significance: We thus present a quantitative guiding rule, a new unifying hallmark of cancer: the cancer cell's transcriptome changes lead to measurable observed transitions of Normalized Shannon Entropy values (as measured by high-throughput technologies). At the same time, tumor cells increment their divergence from the normal tissue profile increasing their disorder via creation of states that we might not directly measure. This unifying hallmark allows, via the the Jensen-Shannon divergence, to identify the arrow of time of the processes from the gene expression profiles, and helps to map the phenotypical and molecular hallmarks of specific cancer subtypes. The deep mathematical basis of the approach allows us to suggest that this principle is, hopefully, of general applicability for other diseases
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
- Author
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- Abbott B
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- Abhayasinghe DK
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- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fbâ1 of sâ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015â2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z â 4â branching fraction is extracted, giving a value of (4.41 ± 0.30) Ă 10â6. Constraints on effective field theory parameters and a model based on a spontaneously broken B â L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Search for anomalous couplings in the W tb vertex from the measurement of double differential angular decay rates of single top quarks produced in the t-channel with the ATLAS detector
- Author
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/10/2015
- Field of study
The electroweak production and subsequent decay of single top quarks is determined by the properties of the Wtb vertex. This vertex can be described by the complex parameters of an effective Lagrangian. An analysis of angular distributions of the decay products of single top quarks produced in the t -channel constrains these parameters simultaneously. The analysis described in this paper uses 4.6 fbâ1 of proton-proton collision data at âs =7 TeV collected with the ATLAS detector at the LHC. Two parameters are measured simultaneously in this analysis. The fraction f 1 of decays containing transversely polarised W bosons is measured to be 0.37 ± 0.07 (stat.âsyst.). The phase ÎŽ â between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be â0.014Ï Â± 0.036Ï (stat.âsyst.). The correlation in the measurement of these parameters is 0.15. These values result in two-dimensional limits at the 95% confidence level on the ratio of the complex coupling parameters g R and V L, yielding Re[g R /V L] â [â0.36, 0.10] and Im[g R /V L] â [â0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
Measurement of the W±Z boson pair-production cross section in pp collisions at âs=13TeV with the ATLAS detector
- Author
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- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
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- 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
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- Netherlands
- Publication date
- 01/01/2016
- Field of study
published_or_final_versio
Measurement of the transverse polarization of Î and ÎÂŻ hyperons produced in proton-proton collisions at âs=7ââTeV using the ATLAS 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
- Adam ER
- Adamczyk 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
- Allison LJ
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- 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
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Aranda CP
- 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
- Artoni G
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Aurousseau M
- Avolio G
- Axen B
- Azuelos G
- Azuma Y
- Baak MA
- Baas AE
- Bacci C
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- Baines JT
- Baker OK
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bannoura AAE
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartos P
- Bassalat A
- Basye A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Battistin M
- Bauer F
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker K
- Becker S
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr K
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
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- Lapoire C
- Laporte JF
- Lari T
- Lassnig M
- Latour BMD
- Laurelli P
- Lavrijsen W
- Law AT
- Laycock P
- Le Dortz O
- Le Guirriec E
- Le Menedeu E
- LeCompte T
- Ledroit-Guillon F
- Lee CA
- Lee H
- Lee L
- Lee SC
- Lefebvre G
- Lefebvre M
- Legger F
- Leggett C
- Lehan A
- Lei X
- Leight WA
- Leisos A
- Leister AG
- Leite MAL
- Leitner R
- Lellouch D
- Lemmer B
- Leney KJC
- Lenz T
- Lenzen G
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- Leone R
- Leone S
- Leonidopoulos C
- Leontsinis S
- Leroy C
- Lester CG
- Lester CM
- Levchenko M
- Leveque J
- Levin D
- Levinson LJ
- Levy M
- Lewis A
- Leyko AM
- Leyton M
- Li B
- Li B
- Li H
- Li HL
- Li L
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- Li S
- Li Y
- Liang Z
- Liao H
- Liberti B
- Lichard P
- Lie K
- Liebal J
- Liebig W
- Limbach C
- Limosani A
- Lin SC
- Lin TH
- Linde F
- Lindquist BE
- Linnemann JT
- Lipeles E
- Lipniacka A
- Lisovyi M
- Liss TM
- Lissauer D
- Lister A
- Litke AM
- Liu B
- Liu D
- Liu J
- Liu JB
- Liu K
- Liu L
- Liu M
- Liu M
- Liu Y
- Livan M
- Llacer MM
- Lleres A
- Lloyd SL
- Lo Sterzo F
- Lobodzinska E
- Loch P
- Lockman WS
- Loebinger FK
- Loevschall-Jensen AE
- Loginov A
- Lohse T
- Lohwasser K
- Lokajicek M
- Long BA
- Long JD
- Long RE
- Looper KA
- Lopes L
- Lopez SP
- Lorenz J
- Losada M
- Loscutoff P
- Lou X
- Lounis A
- Love J
- Love PA
- Lowe AJ
- Lu F
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- Lubatti HJ
- Luci C
- Lucotte A
- Luehring F
- Lukas W
- Luminari L
- Lund-Jensen B
- Lundberg O
- Lungwitz M
- Lynn D
- Lysak R
- Lytken E
- Ma H
- Ma LL
- Maccarrone G
- Macchiolo A
- Machado Miguens J
- Macina D
- Madaffari D
- Madar R
- Maddocks HJ
- Mader WF
- Madsen A
- Maeno M
- Maeno T
- Maettig P
- Maevskiy A
- Magradze E
- Mahboubi K
- Mahlstedt J
- Mahmoud S
- Maiani C
- Maidantchik C
- Maier AA
- Maio A
- Majewski S
- Makida Y
- Makovec N
- Mal P
- Malaescu B
- Malecki P
- Maleev VP
- Malek F
- Mallik U
- Malon D
- Malone C
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- Malyshev VM
- Malyukov S
- Mamuzic J
- Mandelli B
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- Mandic I
- Mandrysch R
- Maneira J
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- Manghi FL
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- Mansoulie B
- Mantifel R
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- Marchand JF
- Marchiori G
- Marcisovsky M
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- Marjanovic M
- Marroquim F
- Marsden SP
- Marshall Z
- Marti LF
- Marti-Garcia S
- Martin B
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- Martin VJ
- Martin-Haugh S
- Martinez H
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- Martinez NL
- Martinez PF
- Martinez VS
- Martyniuk AC
- Marx M
- Marzano F
- Marzin A
- Masetti L
- Mashimo T
- Mashinistov R
- Masik J
- Maslennikov AL
- Massa I
- Massa L
- Massol N
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- Masubuchi T
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- Mattmann J
- Maurer J
- Maxfield SJ
- Maximov DA
- Mazini R
- Mazza SM
- Mazzaferro L
- Mc Goldrick G
- Mc Kee SP
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- McCarthy TG
- McCubbin NA
- McFarlane KW
- Mcfayden JA
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- Milov A
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- Minami Y
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- Ming Y
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- Morley AK
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- Oakham FG
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- Pettersson NE
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- Piacquadio G
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- Plotnikova E
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- Popeneciu GA
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- Radhakrishnan SK
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- Ragusa F
- Rahal G
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- Rurikova Z
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- Ruschke A
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- Tripiana MF
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- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
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- Tudorache V
- Tuna AN
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- Zhemchugov A
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- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2014
- Field of study
The transverse polarization of Î and ÎÂŻ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760ââÎŒbâ1 of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from 5Ă10â5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is â0.010±0.005(stat)±0.004(syst) for Î and 0.002±0.006(stat)±0.004(syst) for ÎÂŻ. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement
Measurement of the photon identification efficiencies with the ATLAS detector using LHC Run-1 data
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- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
© 2016, CERN for the benefit of the ATLAS collaboration.The algorithms used by the ATLAS Collaboration to reconstruct and identify prompt photons are described. Measurements of the photon identification efficiencies are reported, using 4.9 fb- 1 of pp collision data collected at the LHC at s=7 TeV and 20.3 fb- 1 at s=8 TeV. The efficiencies are measured separately for converted and unconverted photons, in four different pseudorapidity regions, for transverse momenta between 10 GeV and 1.5 TeV. The results from the combination of three data-driven techniques are compared to the predictions from a simulation of the detector response, after correcting the electromagnetic shower momenta in the simulation for the average differences observed with respect to data. Data-to-simulation efficiency ratios used as correction factors in physics measurements are determined to account for the small residual efficiency differences. These factors are measured with uncertainties between 0.5% and 10% in 7 TeV data and between 0.5% and 5.6% in 8 TeV data, depending on the photon transverse momentum and pseudorapidity
Measurement of the ttÌW and ttÌZ production cross sections in pp collisions at âs = 8 TeV with the ATLAS detector
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- Zhemchugov A
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- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
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- Zobernig G
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- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
The production cross sections of top-quark pairs in association with massive vector bosons have been measured using data from pp collisions at sâ = 8 TeV. The dataset corresponds to an integrated luminosity of 20.3 fbâÂč collected by the ATLAS detector in 2012 at the LHC. Final states with two, three or four leptons are considered. A fit to the data considering the ttÌW and ttÌZ processes simultaneously yields a significance of 5.0Ï (4.2Ï) over the background-only hypothesis for ttÂŻWttÂŻW (ttÌZ) production. The measured cross sections are ÏttÌW = 369 + 100â91 fb and ÏttÌZ = 176 + 58â52 fb. The background-only hypothesis with neither ttÌW nor ttÌZ production is excluded at 7.1Ï. All measurements are consistent with next-to-leading-order calculations for the ttÌW and ttÌZ processes
Modelling Z â ÏÏ processes in ATLAS with Ï-embedded Z â ΌΌ data
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk 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
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
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- Teuscher RJ
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- Zhemchugov A
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2015
- Field of study
This paper describes the concept, technical realisation and validation of a largely data-driven method to model events with ZâÏÏ decays. In ZâΌΌ events selected from proton-proton collision data recorded at âs=8 TeV with the ATLAS experiment at the LHC in 2012, the Z decay muons are replaced by Ï leptons from simulated ZâÏÏ decays at the level of reconstructed tracks and calorimeter cells. The Ï lepton kinematics are derived from the kinematics of the original muons. Thus, only the well-understood decays of the Z boson and Ï leptons as well as the detector response to the Ï decay products are obtained from simulation. All other aspects of the event, such as the Z boson and jet kinematics as well as effects from multiple interactions, are given by the actual data. This so-called Ï-embedding method is particularly relevant for Higgs boson searches and analyses in ÏÏ final states, where ZarrowÏÏ decays constitute a large irreducible background that cannot be obtained directly from data control samples. In this paper, the relevant concepts are discussed based on the implementation used in the ATLAS Standard Model HâÏÏ analysis of the full datataset recorded during 2011 and 2012
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