223 research outputs found
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
- 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
- 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
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
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- Alimonti G
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- Argyropoulos S
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- 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
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
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- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
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- Yoshihara K
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- Young CJS
- 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
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- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou N
- Zhu CG
- Zhu H
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- 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
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
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
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
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- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
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- Artamonov A
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- Baroncelli A
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- Bindi M
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- Bingul A
- Bini C
- Black CW
- Black JE
- Black KM
- Blackburn D
- Blair RE
- Blanchard J-B
- Blazeka T
- Bloch I
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- Butler B
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- Caminal Armadans R
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- Castelli A
- Castillo Gimenez V
- Castillo IS
- Castillo LRF
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- Castro NF
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- Chernyatin V
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- de Renstrom PAB
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- Deluca C
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- Demirkoz B
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- Deviveiros PO
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- Di Domenico A
- Di Donato C
- Di Girolamo A
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- Di Simone A
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- Ekelof T
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- Enari Y
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- Endner OC
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- Erdmann J
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- Ereditato A
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- Eriksson D
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- Ernis G
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- Errede D
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- Errede S
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- Ertel E
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- Escalier M
- Escalier M
- Esch H
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- Escobar C
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- Espinal Curull X
- Espinal Curull X
- Esposito B
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- Etienne F
- Etienne F
- Etienvre AI
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- Etzion E
- Etzion E
- Evans H
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- Fabbri L
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- Facini G
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- Fajardo LSG
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- Fakhrutdinov RM
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- Falciano S
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- Faltova J
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- Fang Y
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- Fanti M
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- Farbin A
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- Farilla A
- Farilla A
- Farooque T
- Farooque T
- Farrell S
- Farrell S
- Farrington SM
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- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
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- Fassouliotis D
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- Favareto A
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- Fayard L
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- Federic P
- Federic P
- Fedin OL
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- Fedorko W
- 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
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- Fenyuk AB
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- Fernando W
- Fernando W
- Ferrag S
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
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- Ferrari A
- Ferrari A
- Ferrari P
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- Ferrari R
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- Ferrer A
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- Ferrere D
- Ferrere D
- Ferretti C
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- Fiascaris M
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- Fiedler F
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- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
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- Fincke-Keeler M
- Fincke-Keeler M
- Finelli KD
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- Fiolhais MCN
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- Fiorini L
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- Firan A
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- Fischer J
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- Fisher MJ
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- Fitzgerald EA
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- Flechl M
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- Fleck I
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- Fleischmann P
- Fleischmann P
- Fleischmann S
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- Fletcher G
- Fletcher G
- Fletcher GT
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- Flick T
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- 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
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- Fox H
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- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
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- Francis D
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- Franklin M
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- Franz S
- Franz S
- Fraternali M
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- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
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- Froidevaux D
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- Frost JA
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- Fukunaga C
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- Fulsom BG
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- Fuster J
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- Gabizon O
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- Gabrielli A
- Gabrielli A
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- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
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- Galea C
- Galea C
- Galhardo B
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- Gallas EJ
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- Gallo V
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- Gallop BJ
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- Gallus P
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- Gandrajula RP
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- Gao J
- Gao YS
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- Gaob J
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- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
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- Garcia JAB
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- Garcia-Sciveres M
- Gardner RW
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- Garelli N
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- Garonne V
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- Garrido MDMC
- Gatti C
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- Gaudio G
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- Gaur B
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- Gauzzi P
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- Gavrilenko IL
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- Gay C
- Gay C
- Gaycken G
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- Gazis EN
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- Ge P
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- Gecse Z
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- Gee CNP
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- Geerts DAA
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- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
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- Gemme C
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- Gemmell A
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- Genest MH
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- Gentile S
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- George M
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- George S
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- Gerbaudo D
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- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
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- Giacobbe B
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- Giagu S
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- Giangiobbe V
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- Giannetti P
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- Gillman AR
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- Gingrich DM
- Gingrich M
- Giokaris N
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- Giordani MP
- Giordani MP
- Giordano R
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- Giorgi FM
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- Giraud PF
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- Giugni D
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- Giuliani C
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- Giunta M
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- Gjelsten BK
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- Gorini E
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- Gornicki E
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- Goshaw AT
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- Gostkin MI
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √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
Measurements of normalized differential cross sections for tt̄ production in pp collisions at √(s)=7 TeV using the ATLAS detector
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- Yao W-M
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- 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
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
Measurements of normalized differential cross sections for top-quark pair production are presented as a function of the top-quark transverse momentum, and of the mass, transverse momentum, and rapidity of the t¯t system, in proton–proton collisions at a center-of-mass energy of √s=7 TeV. The data set corresponds to an integrated luminosity of 4.6 fb−1, recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one lepton and at least four jets with at least one of the jets tagged as originating from a b-quark. The measured spectra are corrected for detector efficiency and resolution effects and are compared to several Monte Carlo simulations and theory calculations. The results are in fair agreement with the predictions in a wide kinematic range. Nevertheless, data distributions are softer than predicted for higher values of the mass of the t¯t system and of the top-quark transverse momentum. The measurements can also discriminate among different sets of parton distribution functions
Measurement of the transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at √s=7 TeV 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
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- 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
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- Anghinolfi F
- Anh TV
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- Anjos N
- Annovi A
- Antonelli M
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- Antos J
- Anulli F
- Aoki M
- Arabidze G
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- Aranda CP
- Araque JP
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
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- Arslan O
- Artamonov A
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- Bagiacchi P
- Bagnaia P
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- Bain T
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- Baker OK
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- Banerjee S
- Bannoura AAE
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
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- Barnes SL
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- Baroncelli A
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- Bartoldus R
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- Berta P
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- Zaidan R
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- Zhemchugov A
- Zhong J
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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 Λ and Λ¯ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760 μb−1 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 5×10−5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is −0.010±0.005(stat)±0.004(syst) for Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. 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 Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
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- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5 fb[superscript −1] of proton-proton collisions data at √s=7 TeV and 20.3 fb[superscript −1] at √s=8 TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be μ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4 GeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m[subscript H]. They are found to be μ[subscript ggF]=1.32±0.38, μ[subscript VBF]=0.8±0.7, μ[subscript WH]=1.0±1.6, μ[subscript ZH]=0.1[superscript +3.7 subscript −0.1], and μ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript −1.8], for Higgs boson production through gluon fusion, vector-boson fusion, and in association with a W or Z boson or a top-quark pair, respectively. Compared with the previously published ATLAS analysis, the results reported here also benefit from a new energy calibration procedure for photons and the subsequent reduction of the systematic uncertainty on the diphoton mass resolution. No significant deviations from the predictions of the Standard Model are found.European Organization for Nuclear ResearchUnited States. Dept. of EnergyNational Science Foundation (U.S.)Brookhaven National Laborator
Search for high-mass dilepton resonances in pp collisions at s√=8 TeV with the ATLAS detector
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- Meric N
- Mermod P
- Merola L
- Meroni C
- Merritt FS
- Merritt H
- Messina A
- Metcalfe J
- Mete AS
- Meyer C
- Meyer C
- Meyer J
- Meyer J-P
- Middleton RP
- Migas S
- Miguens JM
- Mijovic L
- Mikenberg G
- Mikestikova M
- Mikuz M
- Miller DW
- Mills C
- Milosavljevic MV
- Milov A
- Milstead DA
- Milstein D
- Minaenko AA
- 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
- Mochizuki K
- Moeller V
- Moenig K
- Mohapatra S
- Mohr W
- Molander S
- Moles-Valls R
- Monini C
- Monk J
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- Monticelli F
- Monzani S
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- Moraes A
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- Moreno D
- Morettini P
- Morgenstern M
- Morii M
- Moritz S
- Morley AK
- Mornacchi G
- Morris JD
- Morvaj L
- Moser HG
- Mosidze M
- Moss J
- Mount R
- Mountricha E
- Mouraviev SV
- Moyse EJW
- Muanza S
- Mudd RD
- Mueller F
- Mueller J
- Mueller K
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- Muenstermann D
- Muino PC
- Munwes Y
- Murray WJ
- Musheghyan H
- Musto E
- Myagkov AG
- Myska M
- Nackenhorst O
- Nadal J
- Nagai K
- Nagai R
- Nagai Y
- Nagano K
- Nagarkar A
- Nagasaka Y
- Nagel M
- Nairz AM
- Nakahama Y
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- Nakano I
- Namasivayam H
- Nanava G
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- Nechaeva PY
- Neep TJ
- Negri A
- Negri G
- Negrini M
- Nektarijevic S
- Nelson A
- Nelson TK
- Nemecek S
- Nemethy P
- Nepomuceno AA
- Nessi M
- Neubauer MS
- Neumann M
- Neves RM
- Nevski P
- Newman PR
- Nguyen DH
- Nickerson RB
- Nicolaidou R
- Nicquevert B
- Nielsen J
- Nikiforou N
- Nikiforov A
- Nikolaenko V
- Nikolic-Audit I
- Nikolics K
- Nikolopoulos K
- Nilsson P
- Ninomiya Y
- Nisati A
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- Noccioli EB
- Nodulman L
- Nomachi M
- Nomidis I
- Norberg S
- Nordberg M
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- Nozaki M
- Nozka L
- Ntekas K
- Nunnemann T
- Nurse E
- Nuti F
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- Oakham FG
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- Obermann T
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- Oda S
- Odaka S
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- Ohm CC
- Ohman H
- Ohshima T
- Okamura W
- Okawa H
- Okumura Y
- Okuyama T
- Olariu A
- Olchevski AG
- Oliver Garcia E
- Olszewski A
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- Onofre A
- Onyisi PUE
- Oram CJ
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- Oren Y
- Orestano D
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- Osculati B
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- Otono H
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- Ouellette EA
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- Ouraou A
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- Ouyang Q
- Ovcharova A
- Owen M
- Ozcan VE
- Ozturk N
- Pachal K
- Pacheco Pages A
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- Paganis E
- Pahl C
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- Pan YB
- Panagiotopoulou E
- Pani P
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- Panitkin S
- Pantea D
- Paolozzi L
- Papadopoulou TD
- Papageorgiou K
- Paramonov A
- Paredes BL
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- Parodi AF
- Parodi F
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- Parsons JA
- Parzefall U
- Pasqualucci E
- Passaggio S
- Passeri A
- Pastore F
- Pastore F
- Pasztor G
- Pataraia S
- Patel ND
- Pater JR
- Patricelli S
- Pauly T
- Pearce J
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- Petersen BA
- Petersen TC
- Petit E
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- Petrolo E
- Petrucci F
- Petteni M
- Pettersson NE
- Pezoa R
- Phillips PW
- Piacquadio G
- Pianori E
- Picazio A
- Piccaro E
- Piccinini M
- Piegaia R
- Pignotti DT
- Pilcher JE
- Pilkington AD
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- Plotnikova E
- Plucinski P
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- Pohl D
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- Polesello G
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Pommes K
- Ponce JMI
- 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
- Poulard G
- Poveda J
- Pozdnyakov V
- Pralavorio P
- Pranko A
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- Pravahan R
- Prell S
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- Price LE
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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
- Qian J
- Qin G
- Qin Y
- Quadt A
- Quarrie DR
- Quayle WB
- Queitsch-Maitland M
- Quijada JAM
- Quilty D
- Qureshi A
- Radeka V
- Radescu V
- Radhakrishnan SK
- Radloff P
- Rados P
- Ragusa F
- Rahal G
- Rajagopalan S
- Rammensee M
- Randle-Conde AS
- Rangel-Smith C
- Rao K
- Rauscher F
- Rave S
- Rave TC
- Ravenscroft T
- Raymond M
- Read AL
- Readioff NP
- Reale VP
- Rebuzzi DM
- Redelbach A
- Redlinger G
- Reece R
- Reeves K
- Rehnisch L
- Reisin H
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- Rembser C
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- Ren ZL
- Renaud A
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- Rezanova OL
- Reznicek P
- Rezvani R
- Richter R
- Ridel M
- Rieck P
- Rieger J
- Rijssenbeek M
- Rimoldi A
- Rinaldi L
- Ritsch E
- Riu I
- Rizatdinova F
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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
- Rose M
- 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
- Ryabov YF
- Rybar M
- Rybkin G
- Ryder NC
- Saavedra AF
- 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
- Sampsonidis D
- Sanchez Martinez V
- Sanchez A
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- Sandaker H
- Sandbach RL
- Sander HG
- Sanders MP
- Sandhoff M
- Sandoval C
- Sandoval T
- Sandstroem R
- Sankey DPC
- Sannino F
- Sansoni A
- Santoni C
- Santonico R
- Santos H
- Sapp K
- Sapronov A
- Saraiva JG
- Sarrazin B
- Sartisohn G
- Sasaki O
- Sasaki Y
- Sauvage G
- Sauvan E
- Savard P
- Savu DO
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- Saxon DH
- Saxon J
- Sbarra C
- Sbrizzi A
- Scanlon T
- Scannicchio DA
- Scarcella M
- Schaarschmidt J
- Schacht P
- Schaefer D
- Schaefer R
- Schaefer U
- 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
- Schwanenberger C
- 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
- 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
- Shang R
- Shank JT
- Shao QT
- Shapiro M
- Shatalov PB
- Shaw K
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shiyakova M
- Shmeleva A
- Shochet MJ
- Short D
- Shrestha S
- Shulga E
- Shupe MA
- Shushkevich S
- Sicho P
- Sidiropoulou O
- Sidorov D
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- 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
- 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
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Song HY
- Soni N
- Sood A
- Sopczak A
- Sopko B
- Sopko V
- Sorin 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
- Staerz S
- 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
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stern S
- Stewart GA
- Stillings JA
- Stockton MC
- Stoebe M
- Stoicea G
- Stolte P
- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strandlie A
- Strauss E
- Strauss M
- Strizenec P
- Strohmer R
- Strom DM
- Stroynowski R
- Stucci SA
- Stugu B
- 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
- 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
- Tayalati Y
- Taylor FE
- Taylor GN
- Taylor W
- Tehrani FS
- Teischinger FA
- Teixeira-Dias P
- Temming KK
- Ten Kate H
- Teng PK
- Teoh JJ
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- 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
- Tomoto M
- Tompkins L
- Toms K
- Topilin ND
- Toro RC
- 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
- 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
- Vanguri R
- 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
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Virzi J
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
- Walker R
- Walkowiak W
- Wall R
- Waller P
- Walls FMG
- Walsh B
- Wang C
- Wang C
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang K
- Wang R
- Wang SM
- Wang T
- Wang X
- Wanotayaroj C
- 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 BM
- Webb S
- Weber MS
- Weber SW
- Webster JS
- Weidberg AR
- Weigell P
- Weinert B
- 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
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- 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
- Willis C
- Willocq S
- Wilson A
- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- 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 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
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- 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
- 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
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to dielectron or dimuon final states. Results are presented from an analysis of proton-proton (pp) collisions at a center-of-mass energy of 8 TeV corresponding to an integrated luminosity of 20.3 fb−1 in the dimuon channel. A narrow resonance with Standard Model Z couplings to fermions is excluded at 95% confidence level for masses less than 2.79 TeV in the dielectron channel, 2.53 TeV in the dimuon channel, and 2.90 TeV in the two channels combined. Limits on other model interpretations are also presented, including a grand-unification model based on the E6 gauge group, Z∗ bosons, minimal Z' models, a spin-2 graviton excitation from Randall-Sundrum models, quantum black holes, and a minimal walking technicolor model with a composite Higgs boson
Flavor tagged time-dependent angular analysis of the B0s → J/ψϕ decay and extraction of ΔΓs and the weak phase ϕs in ATLAS
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
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- Agustoni M
- Ahlen SP
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- Alconada Verzini MJ
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- Zhemchugov A
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- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the B0s→J/ψϕ decay parameters, updated to include flavor tagging is reported using 4.9 fb−¹ of integrated luminosity collected by the ATLAS detector from √s=7 TeV pp collisions recorded in 2011 at the LHC. The values measured for the physical parameters are
ϕs=0.12±0.25(stat)±0.05(syst) rad
ΔΓs=0.053±0.021(stat)±0.010(syst) ps−¹
Γs=0.677±0.007(stat)±0.004(syst) ps−¹
|A∥(0)|2=0.220±0.008(stat)±0.009(syst)
|A0(0)|2=0.529±0.006(stat)±0.012(syst)
δ⊥=3.89±0.47(stat)±0.11(syst) rad
where the parameter ΔΓs is constrained to be positive. The S-wave contribution was measured and found to be compatible with zero. Results for ϕs and ΔΓs are also presented as 68% and 95% likelihood contours, which show agreement with the Standard Model expectations
Search for scalar diphoton resonances in the mass range 65-600 GeV with the ATLAS detector in pp collision data at √s = 8 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
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- Yao W-M
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- Yeletskikh I
- 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
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- Yurkewicz A
- 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
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- 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
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A search for scalar particles decaying via narrow resonances into two photons in the mass range 65–600 GeV is performed using 20.3 fb−¹ of √s=8 TeV pp collision data collected with the ATLAS detector at the Large Hadron Collider. The recently discovered Higgs boson is treated as a background. No significant evidence for an additional signal is observed. The results are presented as limits at the 95% confidence level on the production cross section of a scalar boson times branching ratio into two photons, in a fiducial volume where the reconstruction efficiency is approximately independent of the event topology. The upper limits set extend over a considerably wider mass range than previous searches
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
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- 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
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- 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
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
- Atlay NB
- Augsten K
- Aurousseau M
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baak MA
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- Baca MJ
- Bacci C
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- Bagiacchi P
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- Bai Y
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- Baker OK
- Baldin EM
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- Balestri T
- Balli F
- Balunas WK
- Banas E
- Banerjee S
- Bannoura AAE
- Barajas CAC
- Barak L
- Barberio EL
- Barberis D
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- Barisonzi M
- Barklow T
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- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Basye A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
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- Bawa HS
- Beacham JB
- Beattie MD
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- Beauchemin PH
- Beccherle R
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- Bednyakov VA
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- Beermann TA
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- Bell WH
- Bella G
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- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
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- Benhammou Y
- Benjamin DP
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
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- 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 fb−1 of proton-proton collision data at √s =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.⊕syst.). The phase δ − between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be −0.014π ± 0.036π (stat.⊕syst.). 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] ∈ [−0.36, 0.10] and Im[g R /V L] ∈ [−0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
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