983 research outputs found
Reconstructing El Niño Southern Oscillation using data from ships' logbooks, 1815- 1854. Part I: Methodology and Evaluation
- Author
- AJW Catchpole
- C Wang
- CF Ropelewski
- D Barriopedro
- D Gallego
- D Wheeler
- D Wheeler
- D Wheeler
- D Wheeler
- DP Dee
- DS Wilks
- DS Wilks
- DW Stahle
- E Aldrian
- ER Cook
- FB Koek
- GP Können
- GP Können
- Grant R. Bigg
- H Bellenger
- Hannah G. Barrett
- HF Diaz
- J Emile-Geay
- J Gergis
- JM Jones
- Julie M. Jones
- K Braganza
- L Bunge
- M Hannaford
- M KĂŒttel
- ME Mann
- ME Mann
- P Brohan
- PAGES 2 K consortium
- PD Jones
- R GarcĂa-Herrera
- R Neukom
- R Wilson
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
The meteorological information found within shipsâ logbooks is a unique and fascinating source of data for historical climatology. This study uses wind observations from logbooks covering the period 1815 to 1854 to reconstruct an index of El Niño Southern Oscillation (ENSO) for boreal winter (DJF). Statistically-based reconstructions of the Southern Oscillation Index (SOI) are obtained using two methods: principal component regression (PCR) and composite-plus-scale (CPS). Calibration and validation are carried out over the modern period 1979â2014, assessing the relationship between re-gridded seasonal ERA-Interim reanalysis wind data and the instrumental SOI. The reconstruction skill of both the PCR and CPS methods is found to be high with reduction of error skill scores of 0.80 and 0.75, respectively. The relationships derived during the fitting period are then applied to the logbook wind data to reconstruct the historical SOI. We develop a new method to assess the sensitivity of the reconstructions to using a limited number of observations per season and find that the CPS method performs better than PCR with a limited number of observations. A difference in the distribution of wind force terms used by British and Dutch ships is found, and its impact on the reconstruction assessed. The logbook reconstructions agree well with a previous SOI reconstructed from Jakarta rain day counts, 1830â1850, adding robustness to our reconstructions. Comparisons to additional documentary and proxy data sources are provided in a companion paper
Consolidating metabolite identifiers to enable contextual and multi-platform metabolomics data analysis
- Author
- Atsushi Fukushima
- B Usadel
- C Knox
- D Smedley
- DS Wishart
- DW Huang
- EM Lenz
- F Carrari
- Fumio Matsuda
- H Li
- H Pages
- H Redestig
- Henning Redestig
- J Zhang
- K Akiyama
- K Urano
- Kazuki Saito
- M Sud
- Masanori Arita
- Miyako Kusano
- MJvan der Werf
- MP van Iersel
- N Schauer
- P Romero
- P Shannon
- PD Karp
- Plant Metabolic Network
- PubChem
- PubChem
- Q Cui
- R Development Core Team
- R Gentleman
- R Taguchi
- R Williams
- RG CÎté
- T Kind
- T Tokimatsu
- VJ Carey
- VK Mootha
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>Analysis of data from high-throughput experiments depends on the availability of well-structured data that describe the assayed biomolecules. Procedures for obtaining and organizing such meta-data on genes, transcripts and proteins have been streamlined in many data analysis packages, but are still lacking for metabolites. Chemical identifiers are notoriously incoherent, encompassing a wide range of different referencing schemes with varying scope and coverage. Online chemical databases use multiple types of identifiers in parallel but lack a common primary key for reliable database consolidation. Connecting identifiers of analytes found in experimental data with the identifiers of their parent metabolites in public databases can therefore be very laborious.</p> <p>Results</p> <p>Here we present a strategy and a software tool for integrating metabolite identifiers from local reference libraries and public databases that do not depend on a single common primary identifier. The program constructs groups of interconnected identifiers of analytes and metabolites to obtain a local metabolite-centric SQLite database. The created database can be used to map in-house identifiers and synonyms to external resources such as the KEGG database. New identifiers can be imported and directly integrated with existing data. Queries can be performed in a flexible way, both from the command line and from the statistical programming environment R, to obtain data set tailored identifier mappings.</p> <p>Conclusions</p> <p>Efficient cross-referencing of metabolite identifiers is a key technology for metabolomics data analysis. We provide a practical and flexible solution to this task and an open-source program, the metabolite masking tool (MetMask), available at <url>http://metmask.sourceforge.net</url>, that implements our ideas.</p
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
- 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
- Annovi A
- 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
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
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- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
- Bhattarai P
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boutle SK
- Boveia A
- Boyd J
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- Boyko IR
- Bozson AJ
- Bracinik J
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- Briglin DL
- Britton D
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- Brooijmans G
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- Broughton JH
- Bruncko D
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- Buckley AG
- Budagov IA
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
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- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
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- Caforio D
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- Cairo VMM
- Cakir IT
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- Calderini G
- Calfayan P
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- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
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- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Camelia EA
- Cameron D
- Camincher C
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- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
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- Cao T
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- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carter JWS
- Casado MP
- Casha AF
- Casper DW
- Castelijn R
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Cerda Alberich L
- Cerny K
- Cerqueira AS
- Cerri A
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- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
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- Chekanov S
- Chekulaev S
- Chelkov GA
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- Chen J
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- Chen SJ
- Chen X
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- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
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- Chiarella V
- Chiarelli G
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- Chisholm AS
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- Chiu I
- Chiu YH
- Chizhov M
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- Chomont AR
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- Chwastowski JJ
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- Citron ZH
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- Cornell SD
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- Correia AMH
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- Cranmer K
- Crawley SJ
- Creager RA
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cukierman AR
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- Czekierda S
- Czodrowski P
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- David C
- Davidek T
- Davis DR
- Dawson I
- De Asmundis R
- De Beurs M
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- de Jong P
- De la Torre H
- de Lima DEF
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- De Maria A
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Sousa MJDCS
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- Debenedetti C
- Dedovich D
- Deiana AM
- Del Peso J
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- Delitzsch CM
- Dell'Acqua A
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- Delsart PA
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- Demers S
- Demichev M
- Demontigny G
- Denisov SP
- Derendarz D
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- Devesa MR
- Deviveiros PO
- Di Bello FA
- Di Ciaccio A
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- Duschinger D
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- Ecker KM
- Eggleston MG
- Eifert T
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- El Kossei R
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- Falke PJ
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- Farina EM
- Farooque T
- Farrington SM
- Farthouat P
- Fassi F
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- Fawcett WJ
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- Fisher WC
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- Gonzalvo Rodriguez GR
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- Gorbounov PA
- Gordon HA
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- Gottardo CA
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- Grabowska-Bold I
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- Gupta DB
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- Gutschow C
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- Zhemchugov A
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- 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
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- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
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- Yang Z
- Yanush S
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
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- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- 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 inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Abdallah J
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
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- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- 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
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Anastopoulos C
- Ancu LS
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- Anders CF
- Anders G
- Anderson KJ
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- Andrei V
- Anduaga XS
- Angelidakis S
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- Anghinolfi F
- Anisenkov A
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- Antonaki A
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- Aoki M
- Aperio Bella L
- Apolle R
- Arabidze G
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- Arguin JF
- Argyropoulos S
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- Boyko IR
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- Bracinik J
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- Yen AL
- Yilmaz M
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- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Khalek SA
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- Yilmaz M
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- Yorita K
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- Zerwas D
- della Porta GZ
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
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- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fbâ1 of sâ=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan ÎČ < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
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- Abajyan T
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- Abdallah J
- Abdelalim AA
- Abdinov O
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- Yilmaz M
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- Youssef S
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- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
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- Zerwas D
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- Zhemchugov A
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- 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
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or Ï lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, Ï, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan ÎČ in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
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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- 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
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- 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
- Godfrey J
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- Godlewski J
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- Goeringer C
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- Goessling C
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- Goldfarb S
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- Golubkov D
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- Gonalo R
- Goncalo R
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- Gonzalez de la Hoz S
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- Gonzalez Parra G
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- Gonzalez BA
- Gonzalez-Sevilla S
- Gonzalez-Sevilla S
- Goossens L
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- Gorbounov PA
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- Gordon HA
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- 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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- 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
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- 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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- Gutierrez P
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- Gutschow C
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- Guttman N
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- Guyot C
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- Haddad N
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- Haefner P
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- Hanninger GN
- Hansen JB
- Hansen JD
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- Harenberg T
- Harkusha S
- Harper D
- Harrington RD
- Harris OM
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- Hartjes F
- Harvey A
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- Hasegawa Y
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- Hernandez Jimenez Y
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- Kostyukhin VV
- Kotov VM
- Kotwal A
- Kourkoumelis C
- Kouskoura V
- Koutsman A
- Kowalewski R
- Kowalski TZ
- Kozanecki W
- Kozhin AS
- Kral V
- Kramarenko VA
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- Kraus JK
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- Krumshteyn ZV
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- Lanni F
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- Laplace S
- Lapoire C
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- Latour BMD
- Laurelli P
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- Lavrijsen W
- Laycock P
- Le Dortz O
- Le Guirriec E
- Le Menedeu E
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- LeCompte T
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- Lister A
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- Loebinger FK
- Loevschall-Jensen AE
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- Lombardo VP
- Long JD
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- Lopez Mateos D
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- Lou X
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- Luehring F
- Lukas W
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- Lundberg O
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- Macchiolo A
- Macek B
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- 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
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