383 research outputs found
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- 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
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- 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
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- 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
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
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- Azuelos G
- Azuma Y
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- Baccaglioni G
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- Bachacou H
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- Backhaus M
- Badescu E
- Bagnaia P
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- Botterill D
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- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
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- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
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- Collaboration ATLAS
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- Degenhardt J
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- Zhemchugov A
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- 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 √s = 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 pT≥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 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{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 R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Yang UK
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- Yanush S
- Yao L
- Yao Y
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- Ye J
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
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- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
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- Zeitnitz C
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- Zemla A
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- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhou Y
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- Zhuang X
- Zhuravlov V
- 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 fb−1 of s=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 β < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- 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
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- Zobernig G
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- zur Nedden M
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- 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 Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ 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 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ 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 Z′ Models
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
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- Endo M
- Engelmann R
- Engelmann R
- Erdmann J
- Erdmann J
- Ereditato A
- Ereditato A
- Eriksson D
- Eriksson D
- Ernis G
- Ernis G
- Ernst J
- Ernst J
- Ernst M
- Ernst M
- Ernwein J
- Ernwein J
- Errede D
- Errede D
- Errede S
- Errede S
- Ertel E
- Ertel E
- Escalier M
- Escalier M
- Esch H
- Esch H
- Escobar C
- Escobar C
- Espinal Curull X
- Espinal Curull X
- Esposito B
- Esposito B
- Etienne F
- Etienne F
- Etienvre AI
- Etienvre AI
- Etzion E
- Etzion E
- Evans H
- Evans H
- Fabbri L
- Fabbri L
- Facini G
- Facini G
- Fajardo LSG
- Fajardo LSG
- Fakhrutdinov RM
- Fakhrutdinov RM
- Falciano S
- Falciano S
- Faltova J
- Faltova J
- Fang Y
- Fang Y
- Fanti M
- Fanti M
- Farbin A
- Farbin A
- Farilla A
- Farilla A
- Farooque T
- Farooque T
- Farrell S
- Farrell S
- Farrington SM
- Farrington SM
- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
- Fassnacht P
- Fassouliotis D
- Fassouliotis D
- Favareto A
- Favareto A
- Fayard L
- Fayard L
- Federic P
- Federic P
- Fedin OL
- Fedin OL
- Fedorko W
- Fedorko W
- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
- Feigl S
- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
- Feng H
- Fenyuk AB
- Fenyuk AB
- Fernando W
- Fernando W
- Ferrag S
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
- Ferrara V
- Ferrari A
- Ferrari A
- Ferrari P
- Ferrari P
- Ferrari R
- Ferrari R
- Ferrer A
- Ferrer A
- Ferrere D
- Ferrere D
- Ferretti C
- Ferretti C
- Fiascaris M
- Fiascaris M
- Fiedler F
- Fiedler F
- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
- Filthaut F
- Fincke-Keeler M
- Fincke-Keeler M
- Finelli KD
- Finelli KD
- Fiolhais MCN
- Fiolhais MCN
- Fiorini L
- Fiorini L
- Firan A
- Firan A
- Fischer J
- Fischer J
- Fisher MJ
- Fisher MJ
- Fitzgerald EA
- Fitzgerald EA
- Flechl M
- Flechl M
- Fleck I
- Fleck I
- Fleischmann P
- Fleischmann P
- Fleischmann S
- Fleischmann S
- Fletcher G
- Fletcher G
- Fletcher GT
- Fletcher GT
- Flick T
- Flick T
- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
- Flowerdew MJ
- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
- Fournier D
- Fox H
- Fox H
- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
- Franchino S
- Francis D
- Francis D
- Franklin M
- Franklin M
- Franz S
- Franz S
- Fraternali M
- Fraternali M
- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
- Friedrich F
- Froidevaux D
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- Frost JA
- Frost JA
- Fukunaga C
- Fukunaga C
- Fulsom BG
- Fulsom BG
- Fuster J
- Fuster J
- Gabaldon C
- Gabaldon C
- Gabizon O
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
- Gallo V
- Gallop BJ
- Gallop BJ
- Gallus P
- Gallus P
- Galster G
- Galster G
- Gan KK
- Gan KK
- Gandrajula RP
- Gandrajula RP
- Gao J
- Gao YS
- Gao YS
- Gaob J
- Garberson F
- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia C
- Garcia JAB
- Garcia-Sciveres M
- Garcia-Sciveres M
- Gardner RW
- Gardner RW
- Garelli N
- Garelli N
- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
- Gatti C
- Gaudio G
- Gaudio G
- Gaur B
- Gaur B
- Gauthier L
- Gauthier L
- Gauzzi P
- Gauzzi P
- Gavrilenko IL
- Gavrilenko IL
- Gay C
- Gay C
- Gaycken G
- Gaycken G
- Gazis EN
- Gazis EN
- Ge P
- Ge P
- Gecse Z
- Gecse Z
- Gee CNP
- Gee CNP
- Geerts DAA
- Geerts DAA
- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
- Gellerstedt K
- Gemme C
- Gemme C
- Gemmell A
- Gemmell A
- Genest MH
- Genest MH
- Gentile S
- Gentile S
- George M
- George M
- George S
- George S
- Gerbaudo D
- Gerbaudo D
- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
- Ghodbane N
- Giacobbe B
- Giacobbe B
- Giagu S
- Giagu S
- Giangiobbe V
- Giangiobbe V
- Giannetti P
- Giannetti P
- Gianotti F
- Gianotti F
- Gibbard B
- Gibbard B
- Gibson SM
- Gibson SM
- Gilchriese M
- Gilchriese M
- Gillam TPS
- Gillam TPS
- Gillberg D
- Gillberg D
- Gillman AR
- Gillman AR
- Gingrich DM
- Gingrich M
- Giokaris N
- Giokaris N
- Giordani MP
- Giordani MP
- Giordano R
- Giordano R
- Giorgi FM
- Giorgi FM
- Giraud PF
- Giraud PF
- Giugni D
- Giugni D
- Giuliani C
- Giuliani C
- Giunta M
- Giunta M
- Gjelsten BK
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- Gkialas I
- Gkialas I
- Gladilin LK
- Gladilin LK
- Glasman C
- Glasman C
- Glatzer J
- Glatzer J
- Glazov A
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- Goddard JR
- Godfrey J
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- Godlewski J
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- Goeringer C
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- Goessling C
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- Goldfarb S
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- Gonalo R
- Goncalo R
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- Gonzalez Parra G
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- Gonzalez BA
- Gonzalez-Sevilla S
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- Goossens L
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- Gorbounov PA
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- Gordon HA
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- Gorelov I
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- Gorini B
- Gorini B
- Gorini E
- Gorini E
- Gorisek A
- Gorisek A
- Gornicki E
- Gornicki E
- Goshaw AT
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- Gostkin MI
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- Gouighri M
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- Goujdami D
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- Goulette MP
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- Goussiou AG
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- Goy C
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- Gozpinar S
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- Grabas HMX
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- Graber L
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- Grafstroem P
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- Grancagnolo F
- Grancagnolo S
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- Grassi V
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- Gratchev V
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- Gray HM
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- Graziani E
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- Grebenyuk OG
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- Greenwood ZD
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- Griffiths J
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- Grillo AA
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- Griso SP
- Grivaz J-F
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- Grohs JP
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- Grohsjean A
- Gross AGE
- Gross E
- Grosse-Knetter J
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- Grossi GC
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- Groth-Jensen J
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- Guest D
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- Gueta O
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- Guicheney C
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- Guido E
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- Gutierrez P
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- Gutschow C
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- Guttman N
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- Guyot C
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- Gwenlan C
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- Gwilliam CB
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- Haas A
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- Haddad N
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- Haefner P
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- Hanninger GN
- Hansen JB
- Hansen JD
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- Harenberg T
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- Harrington RD
- Harris OM
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- Hartjes F
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- Hasegawa Y
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- Hawkings RJ
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- Haywood SJ
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- Henderson RCW
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- Hernandez Jimenez Y
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- Lapoire C
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- Mercurio KM
- Mergelmeyer S
- Meric N
- Mermod P
- Merola L
- Meroni C
- Merritt FS
- Merritt H
- Messina A
- Metcalfe J
- Mete AS
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- Mijovic L
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- Mikuz M
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- Milov A
- Milstead DA
- Milstein D
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- Minano Moya M
- Minashvili IA
- Mincer AI
- Mindur B
- Mineev M
- Ming Y
- Miotto GL
- Mir LM
- Mirabelli G
- Mitani T
- Mitrevski J
- Mitsou VA
- Mitsui S
- Miucci A
- Miyagawa PS
- Mjornmark JU
- Moa T
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- Monini C
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- Monticelli F
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- Moraes A
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- Mornacchi G
- Morris JD
- Morvaj L
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- Mosidzeb M
- Moss J
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- Mouraviev SV
- Moyse EJW
- Muanza S
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- Muenstermann D
- Munwes Y
- Murray WJ
- Musto E
- Myagkov AG
- Myska M
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- Nadal J
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- Nagai Y
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- Nakano I
- Namasivayam H
- Nanava G
- Narayan R
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- Nechaeva PY
- Nedden MZ
- Neep TJ
- Negri A
- Negri G
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- Nelson A
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- Nemecek S
- Nemethy P
- Nepomuceno AA
- Nessi M
- Neubauer MS
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- Neusiedl A
- Neves RM
- Nevski P
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- Nguyen DH
- Nickerson RB
- Nicolaidou R
- Nicquevert B
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- Nikiforov A
- Nikolaenko V
- Nikolic-Audit I
- Nikolics K
- Nikolopoulos K
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- Ninomiya Y
- Nisati A
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- Nomachi M
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- Nuncio-Quiroz A-E
- Nunnemann T
- Nurse E
- Nuti F
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- O'grady F
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- Oakham FG
- Oberlack H
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- Oliver Garcia E
- Olivito D
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- Oram CJ
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- Oren Y
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- Otono H
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- Ouraou A
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- Paganis E
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- Paige F
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- Panagiotopoulou E
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- Panitkin S
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- Papadopoulou TD
- Papageorgiou K
- Paramonov A
- Paredes BL
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- Parodi AF
- Parodi AF
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- Parsons JA
- Parzefall U
- Pasqualucci E
- Passaggio S
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- Patel ND
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- Petersen BA
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- Petersen TC
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- Petridis A
- Petridou C
- Petrolo E
- Petrucci F
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- Pezoa R
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- Piacquadio G
- Pianori E
- Picazio A
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- Piegaia R
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- Pilkington AD
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- Plotnikova E
- Plucinski P
- Poddar S
- Podlyski F
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- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Pommes K
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- Pontecorvo L
- Pope BG
- Popeneciu GA
- Popovic DS
- Poppleton A
- Portell Bueso X
- Pospelov GE
- Pospisil S
- Potamianos K
- Potrap IN
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- Potter CT
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- Price LE
- Prieur D
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- Proissl M
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- Prokoshin F
- Protopapadaki E
- Protopopescu S
- Proudfoot J
- Przybycien M
- Przysiezniak H
- Ptacek E
- Pueschel E
- Puldon D
- Purohit M
- Puzo P
- Pylypchenko Y
- Pysztor G
- Qian J
- Quadt A
- Quarrie DR
- Quayle WB
- Quijada JAM
- Quilty D
- Qureshi A
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- Radescu V
- Radhakrishnan SK
- Radloff P
- Ragusa F
- Rahal G
- Rajagopalan S
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- Rammes M
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- Randle-Conde AS
- Rangel-Smith C
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- Rebuzzi DM
- Redelbach A
- Redlinger G
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- Reeves K
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- Reinsch A
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- Renaud A
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- Resconi S
- Rezanov OL
- Reznicek P
- Rezvani R
- Richter R
- Ridel M
- Rieck P
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- Rimoldi A
- Rinaldi L
- Ritsch E
- Riu I
- Rizatdinova F
- Rizvi E
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- Robinson JEM
- Robson A
- Roda C
- Rodrigues L
- Roe S
- Rohne O
- Rolli S
- Romaniouk A
- Romano M
- Romeo G
- Romero Adam E
- Rompotis N
- Roos L
- Ros E
- Rosati S
- Rosbach K
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- Rosendahl PL
- Rosenthal O
- Rossetti V
- Rossi E
- Rossi LP
- Rosten R
- Rotaru M
- Roth I
- Rothberg J
- Rousseau D
- Royon CR
- Rozanov A
- Rozen Y
- Ruan X
- Rubbo F
- Rubinskiy I
- Rud VI
- Rudolph C
- Rudolph MS
- Ruehr F
- Ruiz-Martinez A
- Rurikova Z
- Rusakovich NA
- Ruschke A
- Rutherfoord JP
- Ruthmann N
- Ruzicka P
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- Ryder NC
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- Sacerdoti S
- Saddique A
- Sadeh I
- Sadrozinski HF-W
- Sadykov R
- Sakamoto H
- Sakurai Y
- Salamanna G
- Salamon A
- Saleem M
- Salek D
- Salihagic D
- Salnikov A
- Salt J
- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
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- Sanchez Martinez V
- Sanchez A
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- Sandhoff M
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- Sandoval T
- Sandstroem R
- Sankey DPC
- Sansoni A
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- Santonico R
- Santos H
- Sapp K
- Sapronov A
- Saraiva JG
- Sarrazin B
- Sartisohn G
- Sasaki O
- Sasaki Y
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- Sauvan E
- Sauvan JB
- Savard P
- Savu DO
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- Saxon J
- Sbarra C
- Sbrizzi A
- Scanlon T
- Scannicchio DA
- Scarcella M
- Schaarschmidt J
- Schacht P
- Schaefer D
- Schaefer U
- Schaelicke A
- Schaepe S
- Schaetzel S
- Schaffer AC
- Schaile D
- Schamberger RD
- Scharf V
- Schegelsky VA
- Scheirich D
- Schernau M
- Scherzer MI
- Schiavi C
- Schieck J
- Schillo C
- Schioppa M
- Schlenker S
- Schmidt E
- Schmieden K
- Schmitt C
- Schmitt C
- Schmitt S
- Schneider B
- Schnellbach YJ
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock BD
- Schorlemmer ALS
- Schott M
- Schouten D
- Schovancova J
- Schramm S
- Schreyer M
- Schroeder C
- Schroeder TV
- Schuh N
- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwegler P
- Schwemling P
- Schwienhorst R
- Schwindling J
- Schwindt T
- Schwoerer M
- Sciacca FG
- Scifo E
- Sciolla G
- Scott WG
- Scuri F
- Scutti F
- Searcy J
- Sedov G
- Sedykh E
- Seidel SC
- Seiden A
- Seifert F
- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Selbach KE
- Seliverstov DM
- Sellers G
- Seman M
- Semprini-Cesari N
- Serfon C
- Serin L
- Serkin L
- Serre T
- Seuster R
- Severini H
- Sforza F
- Sfyrla A
- Shabalina E
- Shamim M
- Shan LY
- Shank JT
- Shao QT
- Shapiro M
- Shatalov PB
- Shaw K
- Sherwood P
- Shimizu S
- Shimmin CO
- Shimojima M
- Shiyakova M
- Shmeleva A
- Shochet MJ
- Short D
- Shrestha S
- Shulga E
- Shupe MA
- Shushkevich S
- Sicho P
- Sidorov D
- Sidoti A
- Siegert F
- Sijacki D
- Silbert O
- Silva J
- Silva MLG
- Silva MLG
- Silver Y
- Silverstein D
- Silverstein SB
- Simak V
- Simard O
- Simic L
- Simion S
- Simioni E
- Simmons B
- Simoniello R
- Simonyan M
- Sinervo P
- Sinev NB
- Sipica V
- Siragusa G
- Sircar A
- Sisakyan AN
- Sivoklokov SY
- Sjolin J
- Sjursen TB
- Skinnari LA
- Skottowe HP
- Skovpen KY
- Skubic P
- Slater M
- Slavicek T
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith KM
- Smizanska M
- Smolek K
- Snesarev AA
- Snidero G
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Solans CA
- Solar M
- Solc J
- Soldatov EY
- Soldevila U
- Solodkov AA
- Solovyanov OV
- Solovyev V
- Sommer P
- Soni N
- Sood A
- Sopko B
- Sopko V
- Sosebee M
- Soualah R
- Soueid P
- Soukharev AM
- South D
- Spagnolo S
- Spano F
- Spearman WR
- Spighi R
- Spigo G
- Spousta M
- Spreitzer T
- Spurlock B
- St Denis RD
- Stahlman J
- Stamen R
- Stanecka E
- Stanek RW
- Stanescu C
- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Stavina P
- Steele G
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stern S
- Stewart GA
- Stillings JA
- Stockton MC
- Stoebe M
- Stoerig K
- Stoicea G
- Stonjek S
- Stradling AR
- Straessner A
- Strandberg J
- Strandberg S
- Strandlie A
- Strauss E
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Stucci SA
- Stugu B
- Stumer I
- Styles NA
- Su D
- Su J
- Subramania HS
- Subramaniam R
- Succurro A
- Sugaya Y
- Suhr C
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
- Svatos M
- Swedish S
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tam JYC
- Tamsett MC
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanasijczuk AJ
- Tani K
- Tannoury N
- Tapprogge S
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor C
- Taylor FE
- Taylor GN
- Taylor W
- Tehrani FS
- Teischinger FA
- Teixeira-Dias P
- Temming KK
- Ten Kate H
- Teng PK
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- Thoma S
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
- Tipton P
- Tisserant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
- Tomlinson L
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- Topilin ND
- Toro RC
- Torregros EF
- Torregrosa EF
- Torrence E
- Torres H
- Torro Pastor E
- Toth J
- Touchard F
- Tovey DR
- Tran HL
- Trefzger T
- Tremblet L
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Triplett N
- Trischuk W
- Trocme B
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- True P
- Trzebinski M
- Trzupek A
- Tsarouchas C
- Tseng JC-L
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tua A
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Uchida K
- Ueda I
- Ueno R
- Ughetto M
- Ugland M
- Uhlenbrock M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Urbaniec D
- Urquijo P
- Usai G
- Usanova A
- Vacavant L
- Vacek V
- Vachon B
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
- Van der Deijl PC
- van der Geer R
- van der Graaf H
- Van der Leeuw R
- van der Ster D
- van Eldik N
- van Gemmeren P
- van Huysduynen LH
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vannucci F
- Vaque FV
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloso F
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigne R
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Virzi J
- Vitells O
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahrmund S
- Wakabayashi J
- Walder J
- Walker R
- Walkowiak W
- Wall R
- Waller P
- Walls FMG
- Walls FMG
- Walsh B
- Wang C
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- Wang F
- Wang H
- Wang H
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- Wang J
- Wang K
- Wang R
- Wang SM
- Wang T
- Wang X
- Warburton A
- Ward CP
- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
- Watkins PM
- Watson AT
- Watson IJ
- Watson MF
- Watts G
- Watts S
- Waugh AT
- Waugh BM
- Webb S
- Weber MS
- Weber SW
- Webster JS
- Weidberg AR
- Weigell P
- Weingarten J
- Weiser C
- Weits H
- Wells PS
- Wemans ADV
- Wenaus T
- Wendland D
- Weng Z
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Wessels M
- Wetter J
- Whalen K
- White A
- White MJ
- White R
- White S
- Whiteson D
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilkens HG
- Will JZ
- Williams HH
- Williams S
- Willocq S
- Wilson A
- Wilson JA
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wittig T
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wright M
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wyatt TR
- Wynne BM
- Xella S
- Xiao M
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamada M
- Yamaguchi H
- Yamaguchi Y
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- 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 √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,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
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 τ 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, φ, 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 β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
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- Youssef S
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- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
The microsporidian parasites Nosema ceranae and Nosema apis are widespread in honeybee (Apis mellifera) colonies across Scotland
- Author
- C Alaux
- C Alaux
- C Mayack
- C Mayack
- CA Mullin
- CAC Invernizzi
- Christopher Moffat
- Christopher N. Connolly
- D Naug
- D Vanengelsdorp
- DL Cox-Foster
- EH Richards
- EM O’Mahony
- Fiona Highet
- GA Wright
- Geraldine A. Wright
- GR Williams
- GR Williams
- GR Williams
- H Katznelson
- I Fries
- J Klee
- J Moore
- J Stevanovic
- J Whitaker
- J. Daniel Hothersall
- John Durkacz
- Karen A Bollan
- LA Malone
- LAS-DI Garibaldi
- M Higes
- M Higes
- M Higes
- M Higes
- M-P Chauzat
- MA Aizen
- N Gallai
- Nastja Saranzewa
- Nigel E. Raine
- R Martin-Hernandez
- R Martin-Hernandez
- RJ Paxton
- S Fenoy
- S Gisder
- S Plischuk
- SG Potts
- SK Medici
- TP Liu
- WF Huang
- Y Chen
- YP Chen
- Z Zhang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
Nosema ceranae is spreading into areas where Nosema apis already exists. N. ceranae has been reported to cause an asymptomatic infection that may lead, ultimately, to colony collapse. It is thought that there may be a temperature barrier to its infiltration into countries in colder climates. In this study, 71 colonies from Scottish Beekeeper’s Association members have been screened for the presence of N. apis and N. ceranae across Scotland. We find that only 11 of the 71 colonies tested positive for spores by microscopy. However, 70.4 % of colonies screened by PCR revealed the presence of both N. ceranae and N. apis, with only 4.2 or 7 % having either strain alone and 18.3 % being Nosema free. A range of geographically separated colonies testing positive for N. ceranae were sequenced to confirm their identity. All nine sequences confirmed the presence of N. ceranae and indicated the presence of a single new variant. Furthermore, two of the spore-containing colonies had only N. ceranae present, and these exhibited the presence of smaller spores that could be distinguished from N. apis by the analysis of average spore size. Differential quantification of the PCR product revealed N. ceranae to be the dominant species in all seven samples tested. In conclusion, N. ceranae is widespread in Scotland where it exists in combination with the endemic N. apis. A single variant, identical to that found in France (DQ374655) except for the addition of a single nucleotide polymorphism, is present in Scotland
Implementation outcome instruments for use in physical healthcare settings: a systematic review
- Author
- A Adu
- A Liberati
- A Sales
- A Tomotaki
- AL Wilkinson
- Alexandra Ziemann
- B Dow
- BA Rabin
- BJ Powell
- BJ Weiner
- C Malo
- CAC Prinsen
- CB Terwee
- CC Lewis
- CC Lewis
- CD Melas
- CF Stanick
- Christina Daskalopoulou
- CJ Armitage
- CN Baker
- D Garcia-Smith
- D Upton
- D Vanneste
- DAPS Wolf
- DE Beaton
- DT Campbell
- E Murray
- E Park
- E Proctor
- Eleonora Uglik-Marucha
- ES McConnell
- F Ferrando
- GA Aarons
- GA Aarons
- GF Moore
- GL Oliveira
- GM Curran
- H Pinnock
- I Ajzen
- J Everson
- J Razmak
- J-H Wu
- JC Brehaut
- JM Johnston
- K Kroenke
- KL Shaw
- L Abetz
- L Eyre
- L Gao
- L Grooten
- L Kramer
- L Steed
- LA Nydegger
- LADS Diego
- Laura Schatte
- LJ Damschroder
- LJ Damschroder
- Louise Hull
- M Bhor
- M Elf
- M Flanagan
- M Frandes
- M Jaana
- M Kaltenbrunner
- M Marshall
- M Wensing
- MC Brouwers
- MP Eccles
- N Rasoulzadeh
- Nick Sevdalis
- NL Atkinson
- P Glasziou
- P Unni
- PC Dykes
- PS Sockolow
- PV Schaik
- R Schnall
- R Windsor
- RE Glasgow
- RG Martinez
- S Bernhardsson
- S El-Den
- S Joice
- S Phansalkar
- SA Barab
- Sabah Boufkhed
- Silia Vitoratou
- SS Slaghuis
- T Bakas
- T Clinton-McHarg
- T Raykov
- T Willmeroth
- TL Finch
- V Venkatesh
- VD Sousa
- VP Aggelidis
- WC Bevier
- Y Xiao
- Z Khadjesari
- Zarnie Khadjesari
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 18/08/2020
- Field of study
BACKGROUND: Implementation research aims to facilitate the timely and routine implementation and sustainment of evidence-based interventions and services. A glaring gap in this endeavour is the capability of researchers, healthcare practitioners and managers to quantitatively evaluate implementation efforts using psychometrically sound instruments. To encourage and support the use of precise and accurate implementation outcome measures, this systematic review aimed to identify and appraise studies that assess the measurement properties of quantitative implementation outcome instruments used in physical healthcare settings. METHOD: The following data sources were searched from inception to March 2019, with no language restrictions: MEDLINE, EMBASE, PsycINFO, HMIC, CINAHL and the Cochrane library. Studies that evaluated the measurement properties of implementation outcome instruments in physical healthcare settings were eligible for inclusion. Proctor et al.'s taxonomy of implementation outcomes was used to guide the inclusion of implementation outcomes: acceptability, appropriateness, feasibility, adoption, penetration, implementation cost and sustainability. Methodological quality of the included studies was assessed using the COnsensus-based Standards for the selection of health Measurement INstruments (COSMIN) checklist. Psychometric quality of the included instruments was assessed using the Contemporary Psychometrics checklist (ConPsy). Usability was determined by number of items per instrument. RESULTS: Fifty-eight publications reporting on the measurement properties of 55 implementation outcome instruments (65 scales) were identified. The majority of instruments assessed acceptability (n = 33), followed by appropriateness (n = 7), adoption (n = 4), feasibility (n = 4), penetration (n = 4) and sustainability (n = 3) of evidence-based practice. The methodological quality of individual scales was low, with few studies rated as 'excellent' for reliability (6/62) and validity (7/63), and both studies that assessed responsiveness rated as 'poor' (2/2). The psychometric quality of the scales was also low, with 12/65 scales scoring 7 or more out of 22, indicating greater psychometric strength. Six scales (6/65) rated as 'excellent' for usability. CONCLUSION: Investigators assessing implementation outcomes quantitatively should select instruments based on their methodological and psychometric quality to promote consistent and comparable implementation evaluations. Rather than developing ad hoc instruments, we encourage further psychometric testing of instruments with promising methodological and psychometric evidence. SYSTEMATIC REVIEW REGISTRATION: PROSPERO 2017 CRD42017065348
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at root s = 8 TeV with the ATLAS detector (vol 75, 299, 2015)
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- Zhemchugov A
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- Zurzolo G
- 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 fb−1 of √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 EmissT>150 GeV and EmissT>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 presented
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at root s = 8 TeV with the ATLAS detector (vol 75, 299, 2015)
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
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- Chalupkova I
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- Chelkov GA
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- Deviveiros PO
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- Di Domenico A
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- Petersen TC
- Petit E
- Petridis A
- Petridou C
- Petrolo E
- Petrucci F
- Pettersson NE
- Pezoa R
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- Piacquadio G
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- Schorlemmer ALS
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- Schroeder TV
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- Schwartzman A
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- Sekula SJ
- Selbach KE
- Seliverstov DM
- Semprini-Cesari N
- Serfon C
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- Tskhadadze EG
- Tsukerman II
- Tsulaia V
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- Yanush S
- Yao L
- Yao W-M
- Yasu Y
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- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
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- Youssef S
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- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
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- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhang L
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- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhu CG
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zinonos Z
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- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
- …