866 research outputs found
On the origin of the Boson peak in globular proteins
- Author
- Akasaka K
- Ansari A
- Atilgan AR
- Banavar JR
- Buchenau U
- Ciliberti S
- Ciliberti S
- De Los Rios P
- Demirel MC
- Doster W
- Doster W
- F. Piazza
- Frauenfelder H
- Frauenfelder H
- Frauenfelder H
- Frishman D
- Fuentes EJ
- Green JL
- Grigera TS
- Grigera TS
- Götze W
- Haliloglu T
- Hao MH
- Heremans K
- Hinsen K
- Hung AY
- Iben IET
- Karpov VG
- Leyser H
- Martín-Mayor V
- Micheletti C
- Mézard M
- Onuchic JN
- Orecchini A
- P. De Los Rios
- Pawson T
- Piazza F
- S. Ciliberti
- Schirmacher W
- Sheng M
- Tama F
- Taraskin SN
- Tirion MM
- Voigtmann T
- Wyart M
- Xie A
- Yamato T
- Publication venue
- 'Informa UK Limited'
- Publication date
- 09/10/2006
- Field of study
We study the Boson Peak phenomenology experimentally observed in globular
proteins by means of elastic network models. These models are suitable for an
analytic treatment in the framework of Euclidean Random Matrix theory, whose
predictions can be numerically tested on real proteins structures. We find that
the emergence of the Boson Peak is strictly related to an intrinsic mechanical
instability of the protein, in close similarity to what is thought to happen in
glasses. The biological implications of this conclusion are also discussed by
focusing on a representative case study.Comment: Proceedings of the X International Workshop on Disordered Systems,
Molveno (2006
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
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- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
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- Atlay NB
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- 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 Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
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
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- Doglioni C
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- Dubreuil E
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- Ekelof T
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- Enari Y
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- Endner OC
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- Engelmann R
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- Erdmann J
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- Errede D
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- Ertel E
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- Escalier M
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- Esch H
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- Escobar C
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- Espinal Curull X
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- Esposito B
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- Etienne F
- Etienne F
- Etienvre AI
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- Etzion E
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- Evans H
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- Fabbri L
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- Facini G
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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
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- 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
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- Fedin OL
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- Fedorko W
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- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
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- Feligioni L
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- Feng C
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- Feng EJ
- Feng EJ
- Feng H
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- Fenyuk AB
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- Fernando W
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- Ferrag S
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- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
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- Ferrari A
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- Ferrari P
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- Ferrari R
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- Ferrer A
- Ferrer A
- 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
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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
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- 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
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- Fraternali M
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- French ST
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- Friedrich C
- Friedrich C
- Friedrich F
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- Fulsom BG
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- Gabizon O
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- Gabrielli A
- Gabrielli A
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- Gadatsch S
- Gadatsch S
- Gadomski S
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- Gagnon P
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- Galea C
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- 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 YS
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- Garcia BRM
- Garcia C
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- Garcia JAB
- Garcia-Sciveres M
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- 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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- 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
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- 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
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- Ghazlane H
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- Ghodbane N
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- Giacobbe B
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- Giangiobbe V
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- Giannetti P
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- Gianotti F
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- Gillam TPS
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- Gillberg D
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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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- Giraud PF
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- Giugni D
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- Giuliani C
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- Gornicki E
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- Goshaw AT
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- Gostkin MI
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- Yilmaz M
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- 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 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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- 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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- Yilmaz M
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- Yoshihara K
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- Youssef S
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- Yusuff I
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- Zaidan R
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- 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
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- Zhang L
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- 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
- '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 W+W− production in association with one jet in proton–proton collisions at sqrt(s) = 8TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty M
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- 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
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Aranda CP
- Araque JP
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baak MA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Bagiacchi P
- Bagnaia P
- Bai Y
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- Zhemchugov A
- Zhong J
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- Zibell A
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- Zimmermann C
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- Zinonos Z
- Zinser M
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2016
- Field of study
The production of W boson pairs in association with one jet in pp collisions at View the MathML sources=8 TeV is studied using data corresponding to an integrated luminosity of 20.3 fb−1 collected by the ATLAS detector during 2012 at the CERN Large Hadron Collider. The cross section is measured in a fiducial phase-space region defined by the presence of exactly one electron and one muon, missing transverse momentum and exactly one jet with a transverse momentum above 25 GeV and a pseudorapidity of |η|<4.5|η|<4.5. The leptons are required to have opposite electric charge and to pass transverse momentum and pseudorapidity requirements. The fiducial cross section is found to be View the MathML sourceσWWfid,1-jet=136±6(stat)±14(syst)±3(lumi) fb. In combination with a previous measurement restricted to leptonic final states with no associated jets, the fiducial cross section of WW production with zero or one jet is measured to be View the MathML sourceσWWfid,≤1-jet=511±9(stat)±26(syst)±10(lumi) fb. The ratio of fiducial cross sections in final states with one and zero jets is determined to be 0.36±0.050.36±0.05. Finally, a total cross section extrapolated from the fiducial measurement of WW production with zero or one associated jet is reported. The measurements are compared to theoretical predictions and found in good agreement
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
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
- 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
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
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- Alhroob M
- Alimonti G
- Alio L
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- Allbrooke BMM
- Allison LJ
- Allport PP
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- Alviggi MG
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- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- 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
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
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- Abbott B
- Abdallah J
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- 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
Measurement of the W±Z boson pair-production cross section in pp collisions at √s=13TeV with the ATLAS detector
- Author
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- Aad G
- Abbott B
- Abdallah J
- Abdinov O
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- Pollard CS
- Polychronakos V
- Pommes K
- Pontecorvo L
- Pope BG
- Popeneciu GA
- Popovic DS
- Poppleton A
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- Potamianos K
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- Radeka V
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- Rimoldi A
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- Ristic B
- Ritsch E
- Riu I
- Rizatdinova F
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- Rodriguez LP
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- Rogan CS
- Rohne O
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- Romano M
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- Rompotis N
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- Rossi E
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- Rosten R
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- Rozanov A
- Rozen Y
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- Rubbo F
- Rudolph MS
- Ruehr F
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- Rurikova Z
- Rusakovich NA
- Ruschke A
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- Ruthmann N
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- Rybkin G
- Ryu S
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- Rzehorz GF
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- Sadykov R
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- Saha P
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- Saimpert M
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- Salamanna G
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- Salazar Loyola JE
- Salek D
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- Sannino M
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- Saraiva JG
- Sarrazin B
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- Schaffer AC
- Schaile D
- Schamberger RD
- Scharf V
- Schegelsky VA
- Scheirich D
- Schernau M
- Schiavi C
- Schier S
- Schillo C
- Schioppa M
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schneider B
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock BD
- Schopf E
- Schott M
- Schovancova J
- Schramm S
- Schreyer M
- Schroeder TV
- Schuh N
- Schulte A
- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwegler P
- Schweiger H
- Schwemling P
- Schwienhorst R
- Schwindling J
- Schwindt T
- Sciolla G
- Scuri F
- Scutti F
- Searcy J
- Seema P
- Seidel SC
- Seiden A
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- Seixas JM
- Sekhniaidze G
- Sekhon K
- Sekula SJ
- Seliverstov DM
- Semprini-Cesari N
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shaikh NW
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Shatalov PB
- Shaw K
- Shaw SM
- Shcherbakova A
- Shehu CY
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shiyakova M
- Shmeleva A
- Shochet MJ
- Shojaii S
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
- Sickles AM
- Sidebo PE
- Sidiropoulou O
- Sidorov D
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silverstein SB
- Simak V
- Simard O
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- Simion S
- Simioni E
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- Sinervo P
- Sinev NB
- Sioli M
- Siragusa G
- Sivoklokov SY
- Sjolin J
- Skinner MB
- Skottowe HP
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
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- Smiesko J
- Smirnov SY
- Smirnov Y
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- Smizanska M
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- Snesarev AA
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- Sobie R
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- Soh DA
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- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
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- Sorin V
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- Sotiropoulou CL
- Soualah R
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- Spigo G
- Spiller LA
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- St Denis RD
- Stabile A
- Stamen R
- Stamm S
- Stanecka E
- Stanek RW
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- Stanitzki MM
- Stapnes S
- Starchenko EA
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- Starz S
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- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- 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 M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Suchek S
- Sugaya Y
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
- Taccini C
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Taiblum N
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- Takashima R
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tannenwald BB
- Tapia Araya S
- Tapprogge S
- Tarem S
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor AC
- Taylor GN
- Taylor PTE
- Taylor W
- Tehrani FS
- Teischinger FA
- Teixeira-Dias P
- Temming KK
- Temple D
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher J
- Theveneaux-Pelzer T
- Thomas JP
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- Thompson PD
- Thomsen LA
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- Trischuk W
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- Trofymov A
- Troncon C
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- Trovatelli M
- Truong L
- Trzebinski M
- Trzupek A
- Tseng JC-L
- Tsiareshka PV
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsui KM
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turgeman D
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- Tuts PM
- Tyndel M
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Unverdorben C
- Urban J
- Urquijo P
- Urrejola P
- Usai G
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- Vacavant L
- Vacek V
- Vachon B
- Valderanis C
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallecorsa S
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- Van der Deijl PC
- van der Geer R
- van der Graaf H
- van Eldik N
- van Gemmeren P
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
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- Vanguri R
- Vaniachine A
- Vankov P
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasquez JG
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- 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
- Vigani L
- Villa M
- Villar DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vittori C
- Vivarelli I
- Vlachos S
- Vlasak M
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt 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
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- Walder J
- Walker R
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- Wallangen V
- Walls FMG
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- Wardrope DR
- Washbrook A
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- Weber MS
- Weber SW
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- Weidberg AR
- Weinert B
- Weingarten J
- Weiser C
- Weits H
- Wells PS
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- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner MD
- Werner P
- Wessels M
- Wetter J
- Whalen K
- Whallon NL
- Wharton AM
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- White R
- Whiteson D
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- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wittkowski J
- Wolf TMH
- Wolter MW
- Wolters H
- Wong KHY
- Worm SD
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wu M
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yuen SPY
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- Netherlands
- Publication date
- 01/01/2016
- Field of study
published_or_final_versio
- …