14 research outputs found
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
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
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- Armbruster AJ
- Arnaez O
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- Artamonov A
- Artoni G
- Arutinov D
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- Asfandiyarov R
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- Astbury A
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- Atoian G
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- Zhemchugov A
- Zheng S
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- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
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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
Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
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- De Andrade Filho L Manhaes
- de Asmundis R
- De Benedetti A
- De Bruin PH Sales
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- Yigitbasi E
- Yildirim E
- Yildiza H Duran
- Yorita K
- Yoshihara K
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- Yusuff I
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- Zalieckas J
- Zaman A
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- Zanzi D
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- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
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- Zhemchugov A
- Zhou B
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- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
The rejection of forward jets originating from
additional proton–proton interactions (pile-up) is crucial for
a variety of physics analyses at the LHC, including Standard
Model measurements and searches for physics beyond
the Standard Model. The identification of such jets is challenging
due to the lack of track and vertex information in
the pseudorapidity range |η| > 2.5. This paper presents a
novel strategy for forward pile-up jet tagging that exploits
jet shapes and topological jet correlations in pile-up interactions.
Measurements of the per-jet tagging efficiency are
presented using a data set of 3.2 fb−1 of proton–proton collisions
at a centre-of-mass energy of 13 TeV collected with the
ATLAS detector. The fraction of pile-up jets rejected in the
range 2.5 < |η| < 4.5 is estimated in simulated events with
an average of 22 interactions per bunch-crossing. It increases
with jet transverse momentum and, for jets with transverse
momentum between 20 and 50 GeV, it ranges between 49%
and 67% with an efficiency of 85% for selecting hard-scatter
jets. A case study is performed in Higgs boson production
via the vector-boson fusion process, showing that these techniques
mitigate the background growth due to additional
proton–proton interactions, thus enhancing the reach for such
signatures
Epigenetics: At the crossroads between genetic and environmental determinants of disease
- Author
- A Bianco
- A Garg
- A Jahan-Mihan
- A Kozomara
- A Laird
- A Lujambio
- A Rodriguez
- A Vaquero
- AA Gavrilov
- AF Fernández
- AH Ting
- AJ Bannister
- AR Vandiver
- AS Zannas
- AS Zannas
- B Li
- B Weber
- BB Tao
- BL Rodriguez
- BP Lewis
- C Ivorra
- C Jin
- C Mandal
- C Martin
- CD Adams
- CE McCurdy
- CH Waddington
- CK Roberts
- D Al-Hamad
- D Globisch
- D Jjingo
- D Subramaniam
- DE Sterner
- DG Lupiáñez
- DJ Barker
- DK Yadav
- E Ginter
- E Lieberman-Aiden
- EJ Michaud
- ER Smith
- G Ficz
- G Ren
- GA Aguirre
- GA Calin
- GC Burdge
- GR Wyatt
- GW Millington
- H Gowher
- H Ikehata
- H Kimura
- H Masuyama
- H Stroud
- HD Morgan
- HR Kohan-Ghadr
- HW Ryu
- IA Qureshi
- Ian C G Weaver
- IK Sundar
- J Brainard
- J Dekker
- J Krefting
- J Su
- J Winter
- JF Chen
- JF Ndisang
- JI Young
- JJ Wyrick
- JR Dixon
- JS Nanda
- JU Guo
- K Rehman
- K Saliminejad
- K Sjögren
- KA Lillycrop
- KA Lillycrop
- KA Lillycrop
- KD Sinclair
- KG Alberti
- KM Aagaard-Tillery
- KM Radtke
- KW Lee
- L Gesumaria
- L Guelen
- L Keinan-Boker
- L Maitre
- L Mariño-Ramírez
- L Shen
- L Tuddenham
- L Wen
- LP Lim
- M Ballarino
- M Caffo
- M Chekulaeva
- M Esteller
- M Fabbri
- M Kulis
- M Mellén
- M Tahiliani
- MA Parra
- MA Parra
- MC García-Cardona
- MC Myzak
- ME Soler-Oliva
- MF Fraga
- MF Fraga
- MH Kagey
- MH Vickers
- MR Branco
- N Hibio
- N. W. Penn
- P Bhatti
- P Rajendran
- PA Jones
- R Feil
- R Métivier
- R Salemi
- R Teperino
- R Zhang
- RA Copeland
- RA Waterland
- RC Painter
- RP Simon
- RR Kanherkar
- RS Weinstock
- RV Chereji
- S Ecker
- S Friso
- S Karnik
- S Kriaucionis
- S Kriaucionis
- S Nothjunge
- S Singh
- S Zakhari
- SE Mancebo
- SG Jin
- SS Rao
- SV Bach
- SY Roth
- T Gali Ramamoorthy
- T Kouzarides
- TODAY Study Group
- V López
- V Nandakumar
- W Filipowicz
- W Reik
- X Li
- X Wu
- Y Ding
- YF He
- YH Huh
- YK Kim
- Z Hussain
- Z Wang
- Z Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Epigenetic modifications play an essential role in the functional regulation of genes, including their expression. In contrast to the relative stability of the genome, the epigenome varies in a very dynamic way, through what are known as epigenetic mechanisms. These epigenetic modifications are reversible and are conditioned by environmental pressures. The most well-known epigenetic DNA modifications are the methylation of the cytosines present in the context of cytosine-guanine dinucleotides and the posttranslational modification of histones. Several works have reported that events in the early environment are associated with changes in gene expression and biological function and that such changes persist beyond the immediate influence of the stimulus and into adulthood. While the exact molecular mechanisms underlying developmental programming are largely unknown, there is much epidemiological evidence and data from animal studies linking epigenetic modifications with parental lifestyle (e.g., alcohol or tobacco consumption), nutrition, and environmental factors (such as exposure to UV light or heavy metals and stress). Moreover, pre-existing pathologies in the parents (e.g., diabetes, obesity, or metabolic syndrome) can also increase the susceptibility of the offspring to developing certain diseases over the course of their lifetime.Peer reviewe
Search for diphoton events with large missing transverse momentum in 1 fb(-1) of 7 TeV proton-proton collision data with the ATLAS detector ATLAS Collaboration
- Author
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Publication venue
- Publication date
- 01/01/2012
- Field of study
A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb -1 of proton-proton collision data at s=7 TeV recorded with the ATLAS detector. No excess of events was observed above the Standard Model prediction and 95% Confidence Level (CL) upper limits are set on the production cross section for new physics. The limits depend on each model parameter space and vary as follows: Λ<(22-129) fb in the context of a generalised model of gauge-mediated supersymmetry breaking (GGM) with a bino-like lightest neutralino, σ<(27-91) fb in the context of a minimal model of gauge-mediated supersymmetry breaking (SPS8), and σ<(15-27) fb in the context of a specific model with one universal extra dimension (UED). A 95% CL lower limit of 805 GeV, for bino masses above 50 GeV, is set on the GGM gluino mass. Lower limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking scale Λ and on the UED compactification scale 1/R, respectively. These limits provide the most stringent tests of these models to date. © 2012 CERN
Search for diphoton events with large missing transverse momentum in 1 fb(-1) of 7 TeV proton-proton collision data with the ATLAS detector ATLAS Collaboration
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- Yilmazc M
- Yoosoofmiya R
- Yorita K
- Yoshida R
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- Zhaob Z
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- Zieminska D
- Zieminska D
- Zimmermann R
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- Zimmermann S
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- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Ziolkowski M
- Zitoun R
- Zitoun R
- Zivkovic L
- Zivkovic L
- Zmouchko VV
- Zmouchko VV
- Zobernig G
- Zobernig G
- Zoccoli A
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zsenei A
- zur Nedden M
- Zutshi V
- Zutshi V
- Zwalinski L
- Zwalinski Lng X
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2012
- Field of study
A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb(-1) of proton-proton collision data at root s = 7 TeV recorded with the ATLAS detector. No excess of events was observed above the Standard Model prediction and 95% Confidence Level (CL) upper limits are set on the production cross section for new physics. The limits depend on each model parameter space and vary as follows: sigma < (22-129) fb in the context of a generalised model of gauge-mediated supersymmetry breaking (GGM) with a bino-like lightest neutralino, sigma < (27-91) fb in the context of a minimal model of gauge-mediated supersymmetry breaking (SPS8), and sigma < (15-27) fb in the context of a specific model with one universal extra dimension (UED). A 95% CL lower limit of 805 GeV, for bino masses above 50 GeV, is set on the GGM gluino mass. Lower limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking scale Lambda and on the UED compactification scale 1/R, respectively. These limits provide the most stringent tests of these models to date. (C) 2012 CERN. Published by Elsevier B.V. All rights reserved. RI Sivoklokov, Sergey/D-8150-2012; Li, Xuefei/C-3861-2012; Smirnov, Sergei/F-1014-2011; Gladilin, Leonid/B-5226-2011; Barreiro, Fernando/D-9808-2012; Prokoshin, Fedor/E-2795-2012; Fazio, Salvatore /G-5156-2010; Orlov, Ilya/E-6611-2012; Doyle, Anthony/C-5889-2009; Alexa, Calin/F-6345-2010; Moorhead, Gareth/B-6634-2009; Livan, Michele/D-7531-2012; Takai, Helio/C-3301-2012; Petrucci, Fabrizio/G-8348-2012; Jones, Roger/H-5578-2011; Fabbri, Laura/H-3442-2012; Kurashige, Hisaya/H-4916-2012; Villa, Mauro/C-9883-2009; Delmastro, Marco/I-5599-201
Search for diphoton events with large missing transverse momentum in 1 fb<sup>-1</sup> of 7 TeV proton–proton collision data with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Yoosoofmiya R
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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
- Zenisa T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhand Z
- Zhang D
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- Zhangd X
- Zhao L
- Zhao T
- Zhaob Z
- Zhemchugov A
- Zhenga S
- Zhong J
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- Zhou Y
- Zhu H
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- Zhuang X
- Zhub Y
- Zhud CG
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2012
- Field of study
A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb−1of proton–proton collision data at √s=7 TeV recorded with the ATLAS detector. No excess of events was observed above the Standard Model prediction and 95% Confidence Level (CL) upper limits are set on the production cross section for new physics. The limits depend on each model parameter space and vary as follows: σ<(22–129) fb in the context of a generalised model of gauge-mediated supersymmetry breaking (GGM) with a bino-like lightest neutralino, σ<(27–91) fb in the context of a minimal model of gauge-mediated supersymmetry breaking (SPS8), and σ< (15–27) fb in the context of a specific model with one universal extra dimension (UED). A 95% CL lower limit of 805 GeV, for bino masses above 50 GeV, is set on the GGM gluino mass. Lower limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking scale ∧ and on the UED compactification scale 1/R, respectively. These limits provide the most stringent tests of these models to date
Search for diphoton events with large missing transverse momentum in 1 fb(-1) of 7 TeV proton-proton collision data with the ATLAS detector ATLAS Collaboration
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Bogaerts JA
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- Bracinik J
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- Buttinger W
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- Calafiura P
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- Cameron D
- Camillocci ES
- Campana S
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- Carli T
- Carlinoa G
- Carminati L
- Caron S
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- Carter AA
- Carter JR
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- Casado MP
- Cascella M
- Caso C
- Castaneda Miranda E
- Castanheira MTD
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cauz D
- Cavalcanti TP
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- Zhao Z
- Zhaob Z
- Zhemchugov A
- Zhemchugov A
- Zheng S
- Zhenga S
- Zhong J
- Zhong J
- Zhou B
- Zhou B
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- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhuang X
- Zhub Y
- Zhud CG
- Zhuravlov V
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- Zieminska D
- Zieminska D
- Zimmermann R
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Ziolkowski M
- Zitoun R
- Zitoun R
- Zivkovic L
- Zivkovic L
- Zmouchko VV
- Zmouchko VV
- Zobernig G
- Zobernig G
- Zoccoli A
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zsenei A
- zur Nedden M
- Zutshi V
- Zutshi V
- Zwalinski L.
- Zwalinski Lng X
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2012
- Field of study
A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb(-1) of proton-proton collision data at root s = 7 TeV recorded with the ATLAS detector. No excess of events was observed above the Standard Model prediction and 95% Confidence Level (CL) upper limits are set on the production cross section for new physics. The limits depend on each model parameter space and vary as follows: sigma < (22-129) fb in the context of a generalised model of gauge-mediated supersymmetry breaking (GGM) with a bino-like lightest neutralino, sigma < (27-91) fb in the context of a minimal model of gauge-mediated supersymmetry breaking (SPS8), and sigma < (15-27) fb in the context of a specific model with one universal extra dimension (UED). A 95% CL lower limit of 805 GeV, for bino masses above 50 GeV, is set on the GGM gluino mass. Lower limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking scale Lambda and on the UED compactification scale 1/R, respectively. These limits provide the most stringent tests of these models to date. (C) 2012 CERN. Published by Elsevier B.V. All rights reserved
Jet mass and substructure of inclusive jets in sqrt(s) = 7 TeV pp collisions with the ATLAS experiment
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
See paper for full list of authors - 30 pages plus author list (53 pages total), 17 figures, submitted to Journal of High Energy PhysicsRecent studies have highlighted the potential of jet substructure techniques to identify the hadronic decays of boosted heavy particles. These studies all rely upon the assumption that the internal substructure of jets generated by QCD radiation is well understood. In this article, this assumption is tested on an inclusive sample of jets recorded with the ATLAS detector in 2010, which corresponds to 35 pb^-1 of pp collisions delivered by the LHC at sqrt(s) = 7 TeV. In a subsample of events with single pp collisions, measurementes corrected for detector efficiency and resolution are presented with full systematic uncertainties. Jet invariant mass, kt splitting scales and n-subjettiness variables are presented for anti-kt R = 1.0 jets and Cambridge-Aachen R = 1.2 jets. Jet invariant-mass spectra for Cambridge-Aachen R = 1.2 jets after a splitting and filtering procedure are also presented. Leading-order parton-shower Monte Carlo predictions for these variables are found to be broadly in agreement with data. The dependence of mean jet mass on additional pp interactions is also explored
Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector (vol 77, 580, 2017)
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- Aad G
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- Abdallah J
- Abdinov O
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- Yildirim E
- Yildiza HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
SCOAP
Search for top quark decays t -> q H with H -> gamma gamma 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
- Ahmad A
- Ahmadov F
- Aielli G
- 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
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- 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
- 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
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Araque JP
- Arce ATH
- Arguin JF
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
- 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
- Azuelos G
- Azuma Y
- Baak MA
- Bacci C
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee S
- Banfi D
- Bangert A
- Bannoura AAE
- Bansal V
- Bansil HS
- Barajas CAC
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- Berlingen JM
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- Bernius C
- Bernlochner FU
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- Berta P
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- Blazek T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
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- Boek TT
- Boeriu OEV
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- Bogdanchikov AG
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- Boldea V
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- Boumediene D
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- Boutouil S
- Boveia A
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- Boyko IR
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- Bracinik J
- Branchini P
- Brandt A
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- Brau B
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- Braun HM
- Brazzale SF
- Brelier B
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- Brennan AJ
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- Britton D
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- Brock I
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- Bromberg C
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- Bruncko D
- Bruneliere R
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- Bruni A
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- Bryngemark L
- Buanes T
- Buat Q
- Bucci F
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Buehrer F
- Bueso XP
- Bugge L
- Bugge MK
- Bulekov O
- Bundock AC
- Burckhart H
- Burdin S
- Burghgrave B
- Burke S
- Burmeister I
- Busato E
- Buscher D
- Buscher V
- Bussey P
- Bustos ACF
- Buszello CP
- Butler B
- Butler JM
- Butt AI
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Byszewski M
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Calvet D
- Calvet S
- Camarda S
- Cameron D
- Camillocci ES
- Caminada LM
- Campana S
- Campanelli M
- Campoverde A
- Canale V
- Canepa A
- Cantero J
- Cantrill R
- Cao T
- Caprini I
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- Capua M
- Caputo R
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- Carlino G
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- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Castaneda-Miranda E
- Castanheira MTD
- Castelli A
- Castillo IS
- Castillo LRF
- Castro NF
- Catastini P
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cavaliere V
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerio B
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cerv M
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chan K
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Chau CC
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaeva SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
- Chen L
- Chen S
- Chen X
- Chen Y
- Cheng HC
- Cheng Y
- Cheplakov A
- Chernyatin V
- Cheu E
- Chevalier L
- Chiarella V
- Chiefari G
- Childers JT
- Chilingarov A
- Chiodini G
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Chouridou S
- Chow BKB
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Chwastowski JC
- Chytka L
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciocio A
- Cirkovic P
- Citron ZH
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Clarke RN
- Cleland W
- Clemens JC
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coffey L
- Cogan JG
- Coggeshall J
- Cole B
- Cole S
- Colijn AP
- Collins-Tooth C
- Collot J
- Colombo T
- Colon G
- Compostella G
- Coniavitis E
- Conidi MC
- Connell SH
- Connelly IA
- Consonni SM
- Consorti V
- Constantinescu S
- Conta C
- Conti G
- Conventi F
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cote D
- Cottin G
- Coutinho YA
- Cowan G
- Cox BE
- Cranmer K
- Cree G
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cuciuc CM
- Cummings J
- Curatolo M
- Cuthbert C
- Czirr H
- Czodrowski P
- Czyczula Z
- D'Auria S
- D'Onofrio M
- da Costa JBG
- Da Costa JGPF
- Da Via C
- Dabrowski W
- Dafinca A
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Daniells AC
- Dao V
- Darbo G
- Darlea GL
- Darmora S
- Dassoulas JA
- Dattagupta A
- Davey W
- David C
- Davidek T
- Davies E
- Davies M
- Davignon O
- Davison AR
- Davison P
- Davygora Y
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Andrade LM
- de Asmundis R
- De Bruin PHS
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De K
- de la Hoz SG
- De la Torre H
- de Lima DEF
- De Lorenzi F
- De Mendizabal JB
- De Nooij L
- De Pedis D
- De Regie JBD
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De Sousa MJDS
- De Zorzi G
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dechenaux B
- Dedovich DV
- Degenhardt J
- Deigaard I
- Del Peso J
- Del Prete T
- Delgado AT
- Deliot F
- Delitzsch CM
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Dell'Orso M
- Della Pietra M
- della Porta GZ
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demilly A
- Denis RDS
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
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- Diaz MA
- Diehl EB
- Dietrich J
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- Diglio S
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- Doglioni C
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- Dubreuil E
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- El Mourslie RC
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- Enari Y
- Endner OC
- Endo M
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- Erdmann J
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- Esposito B
- Etienvre AI
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- Fajardo LSG
- Fakhrutdinov RM
- Falciano S
- Falla RJ
- Fang Y
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- Farbin A
- Farilla A
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- Farrell S
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- Favareto A
- Fayard L
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- Fedin OL
- Fedorko W
- Fehling-Kaschek M
- Feigl S
- Feligioni L
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- Fenyuk AB
- Ferrag S
- Ferrando BMS
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- Fletcher GT
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- Flowerdew MJ
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- Fournier D
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- Gao J
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- Gardner RW
- Garelli N
- Garonne V
- Garrido MDMC
- Garzon GOY
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- Gaycken G
- Gazis EN
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
A search is performed for flavour-changing neutral currents in the decay of a top quark to an up-type (c, u) quark and a Higgs boson, where the Higgs boson decays to two photons. The proton-proton collision data set used corresponds to 4.7 fb(-1) at root s = 7TeV and 20.3 fb(-1) at root s = 8TeV collected by the ATLAS experiment at the LHC. Top quark pair events are searched for in which one top quark decays to qH and the other decays to bW. Both the hadronic and the leptonic decay modes of the W boson are used. No significant signal is observed and an upper limit is set on the t -> qH branching ratio of 0.79% at the 95% confidence level. The corresponding limit on the tqH coupling combination root lambda(2)(tcH) + root lambda(2)(tuH) is 0.17