984 research outputs found
Aerosol transmission for SARS-CoV-2 in the dental practice. A review by SIdP Covid-19 task-force
- Author
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2020
- Field of study
Scaling properties of protein family phylogenies
- Author
- A Wagner
- A Wagner
- Alejandro Herrada
- AM Simons
- AO Mooers
- AĂ Mooers
- B Burlando
- B Burlando
- BC Daniels
- C Guyer
- C Guyer
- C Roth
- Carlos M Duarte
- D Garlaschelli
- D Lee
- DH Erwin
- DJ Aldous
- DJ Ford
- E HernĂĄndez-GarcĂa
- EA Herrada
- EF Harding
- Emilio HernĂĄndez-GarcĂa
- EV Koonin
- G Apic
- GU Yule
- HM Savage
- I Pinelis
- J Camacho
- J Masel
- JA Cotton
- JA Cotton
- JC Willis
- JFY Brookfield
- JR Banavar
- K Klemm
- KMA Chan
- KP Dial
- LL Cavalli-Sforza
- M Kirkpatrick
- M Sackin
- M Sales-Pardo
- M Stich
- MA Huynen
- MGB Blum
- MGB Blum
- MO Dayhoff
- N Saitou
- NM Luscombe
- O Gascuel
- PM Harrison
- PRA Campos
- R Dawkins
- R Desper
- R Unger
- RE Lenski
- S Guindon
- S Keller-Schmidt
- SB Carroll
- SB Heard
- SB Heard
- SC Morris
- T Grantham
- T Hughes
- TJ Davies
- V Kunin
- VĂctor M EguĂluz
- WJ Bruno
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2011
- Field of study
One of the classical questions in evolutionary biology is how evolutionary
processes are coupled at the gene and species level. With this motivation, we
compare the topological properties (mainly the depth scaling, as a
characterization of balance) of a large set of protein phylogenies with a set
of species phylogenies. The comparative analysis shows that both sets of
phylogenies share remarkably similar scaling behavior, suggesting the
universality of branching rules and of the evolutionary processes that drive
biological diversification from gene to species level. In order to explain such
generality, we propose a simple model which allows us to estimate the
proportion of evolvability/robustness needed to approximate the scaling
behavior observed in the phylogenies, highlighting the relevance of the
robustness of a biological system (species or protein) in the scaling
properties of the phylogenetic trees. Thus, the rules that govern the
incapability of a biological system to diversify are equally relevant both at
the gene and at the species level.Comment: Replaced with final published versio
Ancient Migratory Events in the Middle East: New Clues from the Y-Chromosome Variation of Modern Iranians
- Author
- A GusmĂŁo
- A Keller
- Alessandro Achilli
- AM Cadenas
- Anna Olivieri
- Antonio Torroni
- B Arredi
- B Su
- Baharak Hooshiar Kashani
- C CinnioÄlu
- C Flores
- C Stringer
- CC Lamberg-Karlovsky
- E Bosch
- F Cruciani
- F Cruciani
- Francesca Gandini
- G Hudjashov
- G Passarino
- G Zei
- H Lacau
- HJ Bandelt
- HJ Bandelt
- I Nasidze
- I Nasidze
- J Chiaroni
- JR Luis
- KK Abu-Amero
- L Excoffier
- L Quintana-Murci
- LA Zhivotovsky
- LL Cavalli-Sforza
- LS Whitfield
- M Gimbutas
- M Nei
- M Pala
- M Regueiro
- Massoud Houshmand
- MC Dulik
- MC Terreros
- MF Hammer
- MF Hammer
- MM Lahr
- Mohammad Hossein Sanati
- MT Akbari
- MT Seielstad
- N Al-Zahery
- N Al-Zahery
- Nadia Al-Zahery
- NM Myres
- O Semino
- O Semino
- Ornella Semino
- P Balaresque
- P Briant
- P Shen
- P Soares
- PA Underhill
- PA Underhill
- PA Underhill
- PA Underhill
- PA Underhill
- R Ghirshman
- RD Gray
- RJ King
- RJ King
- RS Wells
- S Amanollahi-Baharvand
- S Farjadian
- S Farjadian
- S Rootsi
- S Sengupta
- Silvia Parolo
- T Kivisild
- TM Karafet
- Toomas Kivisild
- V Battaglia
- Vincenza Battaglia
- Viola Grugni
- Z Lashgary
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2012
- Field of study
Knowledge of high resolution Y-chromosome haplogroup diversification within Iran provides important geographic context regarding the spread and compartmentalization of male lineages in the Middle East and southwestern Asia. At present, the Iranian population is characterized by an extraordinary mix of different ethnic groups speaking a variety of Indo-Iranian, Semitic and Turkic languages. Despite these features, only few studies have investigated the multiethnic components of the Iranian gene pool. In this survey 938 Iranian male DNAs belonging to 15 ethnic groups from 14 Iranian provinces were analyzed for 84 Y-chromosome biallelic markers and 10 STRs. The results show an autochthonous but non-homogeneous ancient background mainly composed by J2a sub-clades with different external contributions. The phylogeography of the main haplogroups allowed identifying post-glacial and Neolithic expansions toward western Eurasia but also recent movements towards the Iranian region from western Eurasia (R1b-L23), Central Asia (Q-M25), Asia Minor (J2a-M92) and southern Mesopotamia (J1-Page08). In spite of the presence of important geographic barriers (Zagros and Alborz mountain ranges, and the Dasht-e Kavir and Dash-e Lut deserts) which may have limited gene flow, AMOVA analysis revealed that language, in addition to geography, has played an important role in shaping the nowadays Iranian gene pool. Overall, this study provides a portrait of the Y-chromosomal variation in Iran, useful for depicting a more comprehensive history of the peoples of this area as well as for reconstructing ancient migration routes. In addition, our results evidence the important role of the Iranian plateau as source and recipient of gene flow between culturally and genetically distinct population
Wave-of-Advance Models of the Diffusion of the Y Chromosome Haplogroup R1b1b2 in Europe
- Author
- A Achilli
- A Torroni
- A Whittle
- AJ Ammerman
- AJ Ammerman
- B Bramanti
- Carles Lalueza-Fox
- F Cruciani
- F Di Giacomo
- G Barbujani
- G Barker
- H Liu
- I Dupanloup
- IJ Wilson
- J Chiaroni
- J Diamond
- L Chikhi
- L Chikhi
- L Morelli
- L Simoni
- LA Zhivotovsky
- LA Zhivotovsky
- LL Cavalli-Sforza
- M Currat
- M Richards
- M Richards
- MA Jobling
- N Ray
- NM Myres
- O Francois
- O François
- O Semino
- Olivier François
- P Balaresque
- P Menozzi
- P Soares
- Per Sjödin
- TR Martin
- W Haak
- W Haak
- W Shi
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Whether or not the spread of agriculture in Europe was accompanied by movements of people is a long-standing question in archeology and anthropology, which has been frequently addressed with the help of population genetic data. Estimates on dates of expansion and geographic origins obtained from genetic data are however sensitive to the calibration of mutation rates and to the mathematical models used to perform inference. For instance, recent data on the Y chromosome haplogroup R1b1b2 (M269) have either suggested a Neolithic origin for European paternal lineages or a more ancient Paleolithic origin depending on the calibration of Y-STR mutation rates. Here we examine the date of expansion and the geographic origin of hgR1b1b2 considering two current estimates of mutation rates in a total of fourteen realistic wave-of-advance models. We report that a range expansion dating to the Paleolithic is unlikely to explain the observed geographical distribution of microsatellite diversity, and that whether the data is informative with respect to the spread of agriculture in Europe depends on the mutation rate assumption in a critical way
On the Analysis of Genome-Wide Association Studies in Family-Based Designs: A Universal, Robust Analysis Approach and an Application to Four Genome-Wide Association Studies
- Author
- A Murphy
- AL Price
- B Devlin
- B Devlin
- C Lange
- C Lange
- C Lange
- C Lange
- C Lange
- C Lange
- Christoph Lange
- Christopher J. O'Donnell
- D Rabinowitz
- DJ Balding
- Edwin K. Silverman
- G Diao
- George T. O'Connor
- GR Abecasis
- H Jiang
- I Ionita-Laza
- Jemma B. Wilk
- JK Pritchard
- K Van Steen
- Kathleen Barnes
- KC Barnes
- LL Cavalli-Sforza
- MP Epstein
- Nicholas J. Schork
- NJ Nagelkerke
- NM Laird
- P Armitage
- PI Lin
- Rasika A. Mathias
- RC Elston
- RS Spielman
- Scott T. Weiss
- Sungho Won
- T Liptak
- WM Chen
- X Zhu
- YH Chen
- YS Aulchenko
- Publication venue
- Public Library of Science
- Publication date
- 01/11/2009
- Field of study
For genome-wide association studies in family-based designs, we propose a new, universally applicable approach. The new test statistic exploits all available information about the association, while, by virtue of its design, it maintains the same robustness against population admixture as traditional family-based approaches that are based exclusively on the within-family information. The approach is suitable for the analysis of almost any trait type, e.g. binary, continuous, time-to-onset, multivariate, etc., and combinations of those. We use simulation studies to verify all theoretically derived properties of the approach, estimate its power, and compare it with other standard approaches. We illustrate the practical implications of the new analysis method by an application to a lung-function phenotype, forced expiratory volume in one second (FEV1) in 4 genome-wide association studies
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Appel
- Arisawa
- Artikov
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- Yeh
- Yi
- Yoh
- Yorita
- Yoshida
- Yu
- Yu
- Yu
- Yun
- Z.
- Zanetti
- Zeng
- Zhou
- Zucchelli
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
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- Abhayasinghe DK
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu CG
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- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- 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 fbâ1 of â 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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at âs = 7 TeV with the ATLAS detector
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- do Vale MAB
- Doan TKO
- Dobos D
- Dobson E
- Doglioni C
- Doherty T
- Dohmae T
- Dolejsi J
- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donati S
- Dondero P
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Santos DR
- Dotti A
- Dova MT
- Doyle AT
- Dris M
- Dubbert J
- Dube S
- Dubreuil E
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Dudziak F
- Duehrssen M
- Dueren M
- Duflot L
- Duguid L
- Dunford M
- Dwuznik M
- Ebke J
- Edson W
- Edwards NC
- Ehrenfeld W
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Moursli A
- El Moursli RC
- Ellert M
- Elles S
- Ellinghaus F
- Ellinghaus F
- Ellis N
- Ellis N
- Elmsheuser J
- Elmsheuser J
- Elsing M
- Elsing M
- Emeliyanov D
- Emeliyanov D
- Enari Y
- Enari Y
- Endner OC
- Endner OC
- Endo M
- Endo M
- Engelmann R
- Engelmann R
- Erdmann J
- Erdmann J
- Ereditato A
- Ereditato A
- Eriksson D
- Eriksson D
- Ernis G
- Ernis G
- Ernst J
- Ernst J
- Ernst M
- Ernst M
- Ernwein J
- Ernwein J
- Errede D
- Errede D
- Errede S
- Errede S
- Ertel E
- Ertel E
- Escalier M
- Escalier M
- Esch H
- Esch H
- Escobar C
- Escobar C
- Espinal Curull X
- Espinal Curull X
- Esposito B
- Esposito B
- Etienne F
- Etienne F
- Etienvre AI
- Etienvre AI
- Etzion E
- Etzion E
- Evans H
- Evans H
- Fabbri L
- Fabbri L
- Facini G
- Facini G
- Fajardo LSG
- Fajardo LSG
- Fakhrutdinov RM
- Fakhrutdinov RM
- Falciano S
- Falciano S
- Faltova J
- Faltova J
- Fang Y
- Fang Y
- Fanti M
- Fanti M
- Farbin A
- Farbin A
- Farilla A
- Farilla A
- Farooque T
- Farooque T
- Farrell S
- Farrell S
- Farrington SM
- Farrington SM
- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
- Fassnacht P
- Fassouliotis D
- Fassouliotis D
- Favareto A
- Favareto A
- Fayard L
- Fayard L
- Federic P
- Federic P
- Fedin OL
- Fedin OL
- Fedorko W
- Fedorko W
- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
- Feigl S
- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
- Feng H
- Fenyuk AB
- Fenyuk AB
- Fernando W
- Fernando W
- Ferrag S
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
- Ferrara V
- Ferrari A
- Ferrari A
- Ferrari P
- Ferrari P
- Ferrari R
- Ferrari R
- Ferrer A
- Ferrer A
- Ferrere D
- Ferrere D
- Ferretti C
- Ferretti C
- Fiascaris M
- Fiascaris M
- Fiedler F
- Fiedler F
- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
- Filthaut F
- Fincke-Keeler M
- Fincke-Keeler M
- Finelli KD
- Finelli KD
- Fiolhais MCN
- Fiolhais MCN
- Fiorini L
- Fiorini L
- Firan A
- Firan A
- Fischer J
- Fischer J
- Fisher MJ
- Fisher MJ
- Fitzgerald EA
- Fitzgerald EA
- Flechl M
- Flechl M
- Fleck I
- Fleck I
- Fleischmann P
- Fleischmann P
- Fleischmann S
- Fleischmann S
- Fletcher G
- Fletcher G
- Fletcher GT
- Fletcher GT
- Flick T
- Flick T
- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
- Flowerdew MJ
- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
- Fournier D
- Fox H
- Fox H
- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
- Franchino S
- Francis D
- Francis D
- Franklin M
- Franklin M
- Franz S
- Franz S
- Fraternali M
- Fraternali M
- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
- Friedrich F
- Froidevaux D
- Froidevaux D
- Frost JA
- Frost JA
- Fukunaga C
- Fukunaga C
- Fulsom BG
- Fulsom BG
- Fuster J
- Fuster J
- Gabaldon C
- Gabaldon C
- Gabizon O
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
- Gallo V
- Gallop BJ
- Gallop BJ
- Gallus P
- Gallus P
- Galster G
- Galster G
- Gan KK
- Gan KK
- Gandrajula RP
- Gandrajula RP
- Gao J
- Gao YS
- Gao YS
- Gaob J
- Garberson F
- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia C
- Garcia JAB
- Garcia-Sciveres M
- Garcia-Sciveres M
- Gardner RW
- Gardner RW
- Garelli N
- Garelli N
- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
- Gatti C
- Gaudio G
- Gaudio G
- Gaur B
- Gaur B
- Gauthier L
- Gauthier L
- Gauzzi P
- Gauzzi P
- Gavrilenko IL
- Gavrilenko IL
- Gay C
- Gay C
- Gaycken G
- Gaycken G
- Gazis EN
- Gazis EN
- Ge P
- Ge P
- Gecse Z
- Gecse Z
- Gee CNP
- Gee CNP
- Geerts DAA
- Geerts DAA
- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
- Gellerstedt K
- Gemme C
- Gemme C
- Gemmell A
- Gemmell A
- Genest MH
- Genest MH
- Gentile S
- Gentile S
- George M
- George M
- George S
- George S
- Gerbaudo D
- Gerbaudo D
- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
- Ghodbane N
- Giacobbe B
- Giacobbe B
- Giagu S
- Giagu S
- Giangiobbe V
- Giangiobbe V
- Giannetti P
- Giannetti P
- Gianotti F
- Gianotti F
- Gibbard B
- Gibbard B
- Gibson SM
- Gibson SM
- Gilchriese M
- Gilchriese M
- Gillam TPS
- Gillam TPS
- Gillberg D
- Gillberg D
- Gillman AR
- Gillman AR
- Gingrich DM
- Gingrich M
- Giokaris N
- Giokaris N
- Giordani MP
- Giordani MP
- Giordano R
- Giordano R
- Giorgi FM
- Giorgi FM
- Giraud PF
- Giraud PF
- Giugni D
- Giugni D
- Giuliani C
- Giuliani C
- Giunta M
- Giunta M
- Gjelsten BK
- Gjelsten BK
- Gkialas I
- Gkialas I
- Gladilin LK
- Gladilin LK
- Glasman C
- Glasman C
- Glatzer J
- Glatzer J
- Glazov A
- Glazov A
- Glonti GL
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- Goddard JR
- Goddard JR
- Godfrey J
- Godfrey J
- Godlewski J
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- Goeringer C
- Goeringer C
- Goessling C
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- Goldfarb S
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- Golubkov D
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- Gomes A
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- Gonalo R
- Goncalo R
- Gonella L
- Gonella L
- Gonzalez de la Hoz S
- Gonzalez de la Hoz S
- Gonzalez Parra G
- Gonzalez Parra G
- Gonzalez BA
- Gonzalez-Sevilla S
- Gonzalez-Sevilla S
- Goossens L
- Goossens L
- Gorbounov PA
- Gorbounov PA
- Gordon HA
- Gordon HA
- Gorelov I
- Gorelov I
- Gorini B
- Gorini B
- Gorini E
- Gorini E
- Gorisek A
- Gorisek A
- Gornicki E
- Gornicki E
- Goshaw AT
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- Gostkin MI
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- Gouighri M
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- Goujdami D
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- Goulette MP
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- Goussiou AG
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- Goy C
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- Gozpinar S
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- Grabas HMX
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- Graber L
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- Grabowska-Bold I
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- Grafstroem P
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- Gramling J
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- Gramstad E
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- Grancagnolo F
- Grancagnolo S
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- Grancagnoloa F
- Grassi V
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- Gratchev V
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- Gray HM
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- Graziani E
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- Grebenyuk OG
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- Greenwood ZD
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- Gregersen K
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- Gregor IM
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- Grenier P
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- Griffiths J
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- Grillo AA
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- Grimm K
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- Grinstein S
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- Gris P
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- Grishkevich YV
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- Griso SP
- Grivaz J-F
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- Grohs JP
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- Grohsjean A
- Gross AGE
- Gross E
- Grosse-Knetter J
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- Grossi GC
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- Groth-Jensen J
- Groth-Jensen J
- Grout ZJ
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- Grybel K
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- Guan L
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- Guescini F
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- Guest D
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- Gueta O
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- Guicheney C
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- Guido E
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- Guillemin T
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- Guindon S
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- Gul U
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- Gumpert C
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- Gunther J
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- Guo J
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- Gutierrez P
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- Gutschow C
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- Guttman N
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- Guyot C
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- Gwenlan C
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- Gwilliam CB
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- Haas A
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- Hadavand HK
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- Haddad N
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- Haefner P
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- Hageboeck S
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- Hajduk Z
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- Hanninger GN
- Hansen JB
- Hansen JD
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- Harenberg T
- Harkusha S
- Harper D
- Harrington RD
- Harris OM
- Harrison PF
- Hartjes F
- Harvey A
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- Hasegawa Y
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- Hawkings RJ
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- Haywood SJ
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- Henderson RCW
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- Hernandez Jimenez Y
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- Herrera CM
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- Kostyukhin VV
- Kotov VM
- Kotwal A
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- Kowalski TZ
- Kozanecki W
- Kozhin AS
- Kral V
- Kramarenko VA
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- Laplace S
- Lapoire C
- Laporte JF
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- Latour BMD
- Laurelli P
- Lavorini V
- Lavrijsen W
- Laycock P
- Le Dortz O
- Le Guirriec E
- Le Menedeu E
- Le BT
- LeCompte T
- Ledroit-Guillon F
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- Lee L
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- Loebinger FK
- Loevschall-Jensen AE
- Loginov A
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- Long JD
- Long RE
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- Luehring F
- Lukas W
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- Lundberg O
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- Macchiolo A
- Macek B
- Macina D
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- 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 âs = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentreâofâmassframeisusedtosuppressthelargemultiâjetbackground.ThecrossâsectionforeventswithahadronicallydecayingWorZboson,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 high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
- Author
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- Abajyan T
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- Abdallah J
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- Zajacova Z
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- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
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- Zhemchugov A
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- Zinonos Z
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- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 23/11/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal ZâČ Models
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