291 research outputs found
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- 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 TP
- 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
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- Amelung C
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- Argyropoulos S
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- Arratia M
- Arslan O
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- Chalupkova I
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Chau CC
- ChavezBarajas CA
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
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- Chernyatin V
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- Chiarella V
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- da Costa JBG
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- Dafinca A
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- De Mendizabal JB
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- 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
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
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- Zaidan R
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- Zanello L
- Zanzi D
- Zeitnitz C
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- Zemla A
- Zengel K
- Zenin O
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- Zerwas D
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- Zhao Z
- Zhemchugov A
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- 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
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
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- Alhroob M
- Alimonti G
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- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
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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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- Zanzi D
- Zaytsev A
- Zeitnitz C
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- Zemla A
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- Zhemchugov A
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- Zieminska D
- Zimine NI
- Zimmermann C
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- Zimmermann S
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- 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 an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state with two bquarks and two tau leptons in proton-proton collisions at root s=13 TeV The CMS Collaboration
- Author
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for an exotic decay of the Higgs boson to a pair of light pseudoscalar bosons is performed for the first time in the final state with two b quarks and two tau leptons. The search is motivated in the context of models of physics beyond the standard model (SM), such as two Higgs doublet models extended with a complex scalar singlet (2HDM + S), which include the next-to-minimal supersymmetric SM (NMSSM). The results are based on a data set of proton-proton collisions corresponding to an integrated luminosity of 35.9 fb(-1), accumulated by the CMS experiment at the LHC in 2016 at a center-of-mass energy of 13 TeV. Masses of the pseudoscalar boson between 15 and 60 GeVare probed, and no excess of events above the SM expectation is observed. Upper limits between 3 and 12% are set on the branching fraction B(h -> aa -> 2 tau 2b) assuming the SM production of the Higgs boson. Upper limits are also set on the branching fraction of the Higgs boson to two light pseudoscalar bosons in different 2HDM + S scenarios. Assuming the SM production cross section for the Higgs boson, the upper limit on this quantity is as low as 20% for a mass of the pseudoscalar of 40 GeV in the NMSSM. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
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- Zuolo D
- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Search for Higgs boson pair production in the gamma gamma b(b)over-bar final state in pp collisions at root s=13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
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- Abu Zeid S
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search is presented for the production of a pair of Higgs bosons, where one decays into two photons and the other one into a bottom quark-antiquark pair. The analysis is performed using proton-proton collision data at root s = 13 TeV recorded in 2016 by the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1) . The results are in agreement with standard model (SM) predictions. In a search for resonant production, upper limits are set on the cross section for new spin-0 or spin-2 particles. For the SM-like nonresonant production hypothesis, the data exclude a product of cross section and branching fraction larger than 2.0 fb at 95% confidence level (CL), corresponding to about 24 times the SM prediction. Values of the effective Higgs boson self-coupling K X are constrained to be within the range -11 < K-lambda < 17 at 95% CL, assuming all other Higgs boson couplings are at their SM value. The constraints on K-lambda, are the most restrictive to date. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Search for the X(5568) State Decaying into B-s(0)pi(+/-) in Proton-Proton Collisions at root s=8 TeV
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- Yu SS
- Yuan L
- Yuldashev BS
- Yumiceva F
- Yusli MN
- Zabel J
- Zabi A
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- Zahid S
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- Zenz SC
- Zeuner WD
- Zevi Della Porta G
- Zeyrek M
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- Zhang A
- Zhang F
- Zhang H
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- Zhang Z
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- Zhemchugov E
- Zhiltsov V
- Zhokin A
- Zhu DH
- Zhu RY
- Zhukov V
- Zientek M
- Zobec J
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- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Álvarez Fernández A
- Publication venue
- Publication date
- 01/01/2017
- Field of study
A search for resonancelike structures in the B-s(0)pi(+/-) invariant mass spectrum is performed using proton-proton collision data collected by the CMS experiment at the LHC at root s = 8 TeV, corresponding to an integrated luminosity of 19.7 fb(-1). The B-s(0) mesons are reconstructed in the decay chain B-s(0) -> J/Psi phi, with J/Psi -> mu(+) mu(-) and phi -> K+K-. The B-s(0)pi(+/-) invariant mass distribution shows no statistically significant peaks for different selection requirements on the reconstructed B-s(0) and pi(+/-) candidates. Upper limits are set on the relative production rates of the X(5568) and B-s(0) states times the branching fraction of the decay X(5568)(+/-) -> B-s(0)pi(+/-). In addition, upper limits are obtained as a function of the mass and the natural width of possible exotic states decaying into B-s(0)pi(+/-).Peer reviewe
Measurement of inclusive very forward jet cross sections in proton-lead collisions at \sqrt{sNN} = 5:02 TeV
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- Yilmaz Y
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- Yusli MN
- Zabel J
- Zabi A
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- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zevi Della Porta G
- Zeyrek M
- Zghiche A
- Zhang A
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- Zhaozhong S
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2019
- Field of study
Measurements of differential cross sections for inclusive very forward jet production in proton-lead collisions as a function of jet energy are presented. The data were collected with the CMS experiment at the LHC in the laboratory pseudorapidity range −6.6 < η < −5.2. Asymmetric beam energies of 4 TeV for protons and 1.58 TeV per nucleon for Pb nuclei were used, corresponding to a center-of-mass energy per nucleon pair of \sqrt{sNN} = 5:02 TeV. Collisions with either the proton (p+Pb) or the ion (Pb+p) traveling towards the negative η hemisphere are studied. The jet cross sections are unfolded to stable-particle level cross sections with p_{T} ≳ 3 GeV, and compared to predictions from various Monte Carlo event generators. In addition, the cross section ratio of p+Pb and Pb+p data is presented. The results are discussed in terms of the saturation of gluon densities at low fractional parton momenta. None of the models under consideration describes all the data over the full jet-energy range and for all beam configurations. Discrepancies between the differential cross sections in data and model predictions of more than two orders of magnitude are observed
Iron Behaving Badly: Inappropriate Iron Chelation as a Major Contributor to the Aetiology of Vascular and Other Progressive Inflammatory and Degenerative Diseases
- Author
- A Abbott
- A Abou-Raya
- A Aljandali
- A Ambesi-Impiombato
- A Aydin
- A Balcerczyk
- A Besarab
- A Brzezinski
- A Campbell
- A Carrillo-Vico
- A Cavalli
- A Chattopadhyay
- A Chattopadhyay
- A Cherubini
- A Dey
- A Doms
- A Donovan
- A Donovan
- A Dávalos
- A Gaeta
- A Garny
- A Gnjec
- A Gomes
- A Gopalakrishnan
- A Hald
- A Henney
- A Hirayama
- A Hoffmann
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- The Long-Term Intervention with Pravastatin in Ischaemic Disease (LIPID) Study Group
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- Publication venue
- Publication date
- 09/08/2008
- Field of study
The production of peroxide and superoxide is an inevitable consequence of
aerobic metabolism, and while these particular "reactive oxygen species" (ROSs)
can exhibit a number of biological effects, they are not of themselves
excessively reactive and thus they are not especially damaging at physiological
concentrations. However, their reactions with poorly liganded iron species can
lead to the catalytic production of the very reactive and dangerous hydroxyl
radical, which is exceptionally damaging, and a major cause of chronic
inflammation. We review the considerable and wide-ranging evidence for the
involvement of this combination of (su)peroxide and poorly liganded iron in a
large number of physiological and indeed pathological processes and
inflammatory disorders, especially those involving the progressive degradation
of cellular and organismal performance. These diseases share a great many
similarities and thus might be considered to have a common cause (i.e.
iron-catalysed free radical and especially hydroxyl radical generation). The
studies reviewed include those focused on a series of cardiovascular, metabolic
and neurological diseases, where iron can be found at the sites of plaques and
lesions, as well as studies showing the significance of iron to aging and
longevity. The effective chelation of iron by natural or synthetic ligands is
thus of major physiological (and potentially therapeutic) importance. As
systems properties, we need to recognise that physiological observables have
multiple molecular causes, and studying them in isolation leads to inconsistent
patterns of apparent causality when it is the simultaneous combination of
multiple factors that is responsible. This explains, for instance, the
decidedly mixed effects of antioxidants that have been observed, etc...Comment: 159 pages, including 9 Figs and 2184 reference
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
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
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- 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
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