221 research outputs found
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
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- Abulaiti Y
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- Achkar B
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu C
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- 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 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
FOX-2 Dependent Splicing of Ataxin-2 Transcript Is Affected by Ataxin-1 Overexpression
- Author
- A Affaitati
- A Gottschalk
- A Matilla-Duenas
- AF Neuwald
- BJ Blencowe
- BR Graveley
- C Bettencourt
- C de Chiara
- C de Chiara
- C de Chiara
- C Le Guiner
- C Li
- C Papin
- C Zhang
- CC Tsai
- Christian Kaehler
- CL Martin
- DD Einum
- ET Wang
- Franziska Welzel
- GM Harris
- GS Wang
- GW Yeo
- H Konig
- H Kuroyanagi
- H Shibata
- Hans Lehrach
- HT Orr
- HY Zoghbi
- HY Zoghbi
- I Al-Ramahi
- I Lastres-Becker
- IA Klement
- J Branco
- J Goto
- J Lim
- J Lim
- JA Lee
- JF Caceres
- JG Underwood
- KE Lukong
- L Corsini
- L Hallen
- Linda Hallen
- LM Dember
- M Ralser
- M Ralser
- Melanie Isau
- ML Hamshere
- MM Denis
- N Delestienne
- N Lopez-Bigas
- NL Kedersha
- P Anderson
- P Fernandez-Funez
- Pedro Fernandez-Funez
- PJ Skinner
- PS Reddy
- R Truant
- S Banfi
- S Irwin
- S Kang
- S Lale
- S Nakahata
- S Sahba
- S Yue
- SJ Kim
- Sylvia Krobitsch
- T Rich
- T Tsunemi
- U Nonhoff
- W Jiang
- Y Lee
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
Alternative splicing is a fundamental posttranscriptional mechanism for controlling gene expression, and splicing defects have been linked to various human disorders. The splicing factor FOX-2 is part of a main protein interaction hub in a network related to human inherited ataxias, however, its impact remains to be elucidated. Here, we focused on the reported interaction between FOX-2 and ataxin-1, the disease-causing protein in spinocerebellar ataxia type 1. In this line, we further evaluated this interaction by yeast-2-hybrid analyses and co-immunoprecipitation experiments in mammalian cells. Interestingly, we discovered that FOX-2 localization and splicing activity is affected in the presence of nuclear ataxin-1 inclusions. Moreover, we observed that FOX-2 directly interacts with ataxin-2, a protein modulating spinocerebellar ataxia type 1 pathogenesis. Finally, we provide evidence that splicing of pre-mRNA of ataxin-2 depends on FOX-2 activity, since reduction of FOX-2 levels led to increased skipping of exon 18 in ataxin-2 transcripts. Most striking, we observed that ataxin-1 overexpression has an effect on this splicing event as well. Thus, our results demonstrate that FOX-2 is involved in splicing of ataxin-2 transcripts and that this splicing event is altered by overexpression of ataxin-1
Transcriptome Analysis of the Model Protozoan, Tetrahymena thermophila, Using Deep RNA Sequencing
- Author
- A Agarwal
- A Conesa
- A Labadorf
- A Mortazavi
- AJ Matlin
- AK Ramani
- AL Delcher
- AP Turkewitz
- B Modrek
- B Modrek
- BJ Loftus
- BR Graveley
- BR Graveley
- BT Wilhelm
- C Ellenrieder
- C Trapnell
- C Trapnell
- Chengjie Fu
- CW Greider
- DJ Asai
- DJ Asai
- DJ Asai
- DL Black
- Dongxia Yuan
- DY Shen
- E Chacko
- E Orias
- Eduardo Orias
- EH Blackburn
- ET Wang
- F Martin
- G Glockner
- GJ Zhang
- H Keren
- J Lu
- J Xiong
- JA Eisen
- JC Marioni
- JE Brownell
- Jie Xiong
- Jonathan H. Badger
- K Kruger
- K Mochizuki
- K Sorber
- L Aronica
- L Pan
- Lei Wang
- M Ashburner
- M Kuiper
- M Sultan
- MA Gorovsky
- Miao Tian
- MJ Robinson
- MT Couvillion
- O Jaillon
- P Rice
- QM Mitrovich
- RF Luco
- RJ Davis
- RS Coyne
- S Marguerat
- S Ortega
- S Stamm
- SA Filichkin
- SD Taverna
- SM Berget
- TD Otto
- TW Nilsen
- U Nagalakshmi
- VM Bruno
- W Miao
- Wei Miao
- Xingyi Lu
- Y Xing
- YN Yang
- Yue Chang
- Z Wang
- Zhemin Zhou
- Zhigang Zhou
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
Background: The ciliated protozoan Tetrahymena thermophila is a well-studied single-celled eukaryote model organism for cellular and molecular biology. However, the lack of extensive T. thermophila cDNA libraries or a large expressed sequence tag (EST) database limited the quality of the original genome annotation. Methodology/Principal Findings: This RNA-seq study describes the first deep sequencing analysis of the T. thermophila transcriptome during the three major stages of the life cycle: growth, starvation and conjugation. Uniquely mapped reads covered more than 96 % of the 24,725 predicted gene models in the somatic genome. More than 1,000 new transcribed regions were identified. The great dynamic range of RNA-seq allowed detection of a nearly six order-of-magnitude range of measurable gene expression orchestrated by this cell. RNA-seq also allowed the first prediction of transcript untranslated regions (UTRs) and an updated (larger) size estimate of the T. thermophila transcriptome: 57 Mb, or about 55 % of the somatic genome. Our study identified nearly 1,500 alternative splicing (AS) events distributed over 5.2 % of T. thermophila genes. This percentage represents a two order-of-magnitude increase over previous EST-based estimates in Tetrahymena. Evidence of stage-specific regulation of alternative splicing was also obtained. Finally, our study allowed us to completely confirm about 26.8 % of the genes originally predicted by the gene finder, to correct coding sequence boundaries an
Pan-cancer analysis of whole genomes
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- Aburatani
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- Birney E. f
- Birrer M. r
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- bw Papatheodorou
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- by Siebert
- Byrne N. J. n
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- Cafferkey A. f
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- Campbell P. J. a
- Campo
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- cd Ossowski
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- cg Sabarinathan
- Chadwick
- Chakravarty
- Chalmers
- Chan
- Chan-Seng-Yue
- Chandan
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- Chanock
- Chateigner A. n
- Chatterjee
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- Chen
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- Cho J. b
- Choi
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- The ICGC/TCGA Pan-Cancer Analysis of Whole Genomes Consortium View Correspondence (jump link)
- Thiessen
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- Y. rg
- Y. rj
- Y. rm
- Y. S. jf
- Y. uz
- Y. vr
- Y. wt
- Y. yc
- ya Al-Ahmadie
- Yachida
- Yamaguchi
- Yamaguchi T. N. k
- Yamamoto
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- Yang
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- z ah
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- zd Gershenwald
- Zenklusen
- Zeps
- zf Ghossein
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang H. b
- Zhao
- Zheng
- Zhou
- Zhou
- Zhu
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- zi zj
- zm Jayaseelan
- Zou
- Zou
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- zw Lewis
- Ó. A. th
- Ø. sk
- Publication venue
- Publication date
- 11/12/2019
- Field of study
Cancer is driven by genetic change, and the advent of massively parallel sequencing has enabled systematic documentation of this variation at the whole-genome scale(1-3). Here we report the integrative analysis of 2,658 whole-cancer genomes and their matching normal tissues across 38 tumour types from the Pan-Cancer Analysis of Whole Genomes (PCAWG) Consortium of the International Cancer Genome Consortium (ICGC) and The Cancer Genome Atlas (TCGA). We describe the generation of the PCAWG resource, facilitated by international data sharing using compute clouds. On average, cancer genomes contained 4-5 driver mutations when combining coding and non-coding genomic elements; however, in around 5% of cases no drivers were identified, suggesting that cancer driver discovery is not yet complete. Chromothripsis, in which many clustered structural variants arise in a single catastrophic event, is frequently an early event in tumour evolution; in acral melanoma, for example, these events precede most somatic point mutations and affect several cancer-associated genes simultaneously. Cancers with abnormal telomere maintenance often originate from tissues with low replicative activity and show several mechanisms of preventing telomere attrition to critical levels. Common and rare germline variants affect patterns of somatic mutation, including point mutations, structural variants and somatic retrotransposition. A collection of papers from the PCAWG Consortium describes non-coding mutations that drive cancer beyond those in the TERT promoter(4); identifies new signatures of mutational processes that cause base substitutions, small insertions and deletions and structural variation(5,6); analyses timings and patterns of tumour evolution(7); describes the diverse transcriptional consequences of somatic mutation on splicing, expression levels, fusion genes and promoter activity(8,9); and evaluates a range of more-specialized features of cancer genomes(8,10-18).Peer reviewe
Dijet Resonance Search with Weak Supervision Using root S=13 TeV pp Collisions in the ATLAS Detector
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- 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
- 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
- Ahmad A
- Ahmadov F
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- 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
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- Aliev M
- Alimonti G
- Allaire C
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- Amaral Coutinho Y
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- Andreazza A
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- Angelidakis S
- Angerami A
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- Blumenschein U
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- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
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- Boisvert V
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- Bolz AE
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- Borisov A
- Borissov G
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- Brost E
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
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- Budagov IA
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- Bugge MK
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- Bullard BA
- Burch TJ
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- Burgard CD
- Burger AM
- Burghgrave B
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- 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
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
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- Camarda S
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- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
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- Campana S
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- Canesse A
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- Cao T
- Cao Y
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- Carlino G
- Carlson BT
- Carlson EM
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- Carter TM
- Casado MP
- Casha AF
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavallaro E
- Cavasinni V
- Celebi E
- Celli F
- Cerda Alberich L
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- Chargeishvili B
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- Chelkov GA
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- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
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- Chiu I
- Chiu YH
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- Chow YS
- Christopher LD
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- Cinca D
- Cindro V
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- Ciocio A
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- De Asmundis R
- De Beurs M
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- de Jong P
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- de Renstrom PAB
- De Salvo A
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- Deviveiros PO
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- Di Donato C
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- Di Gregorio G
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- Knue A
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- Koehler NM
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- Komarek T
- Kondo T
- Kong AXY
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- Kotwal A
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- Kourkoumelis C
- Kourlitis E
- Kouskoura V
- Kowalewska AB
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 25/09/2020
- Field of study
This Letter describes a search for narrowly resonant new physics using a machine-learning anomaly
detection procedure that does not rely on signal simulations for developing the analysis selection. Weakly
supervised learning is used to train classifiers directly on data to enhance potential signals. The targeted
topology is dijet events and the features used for machine learning are the masses of the two jets. The
resulting analysis is essentially a three-dimensional search A → BC, for mA ∼ OðTeVÞ, mB; mC ∼
Oð100 GeVÞ and B, C are reconstructed as large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two jets. The full run 2 ffiffi
s p ¼ 13 TeV pp collision
dataset of 139 fb−1 recorded by the ATLAS detector at the Large Hadron Collider is used for the search.
There is no significant evidence of a localized excess in the dijet invariant mass spectrum between 1.8 and
8.2 TeV. Cross-section limits for narrow-width A, B, and C particles vary with mA, mB, and mC. For
example, when mA ¼ 3 TeV and mB ≳ 200 GeV, a production cross section between 1 and 5 fb is
excluded at 95% confidence level, depending on mC. For certain masses, these limits are up to 10 times
more sensitive than those obtained by the inclusive dijet search. These results are complementary to the
dedicated searches for the case that B and C are standard model boson
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
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- Zhemchugov A
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- Zinonos Z
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
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- Coimbra AEC
- Cole B
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- Columbie JMC
- Connell SH
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- Conventi F
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- Cornell SD
- Corpe LD
- Corradi M
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- de Renstrom PAB
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- Dedovich DV
- Degens J
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- Zenger DT
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- Zerwas D
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- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu Y
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
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- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Search for heavy neutral Higgs bosons produced in association with b-quarks and decaying into b-quarks at root s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- 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
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
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- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
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- Zhemchugov A
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 13/08/2020
- Field of study
A search for heavy neutral Higgs bosons produced in association with one or two
b
-quarks and decaying to
b
-quark pairs is presented using
27.8
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015 and 2016. No evidence of a signal is found. Upper limits on the heavy neutral Higgs boson production cross section times its branching ratio to
b
¯
b
are set, ranging from 4.0 to 0.6 pb at 95% confidence level over a Higgs boson mass range of 450 to 1400 GeV. Results are interpreted within the two-Higgs-doublet model and the minimal supersymmetric Standard Model
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
- Author
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- Yildiz HD
- Yin P
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- Yoshihara K
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- Zahreddine J
- Zaitsev AM
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- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
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- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhou H
- Zhou M
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- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb−1 of s√ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015–2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z → 4ℓ branching fraction is extracted, giving a value of (4.41 ± 0.30) × 10−6. Constraints on effective field theory parameters and a model based on a spontaneously broken B − L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Measurement of the inclusive cross-section for the production of jets in association with a Z boson in proton-proton collisions at 8 TeV using the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- 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 TP
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
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- Alshehri AA
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- Alvarez Piqueras D
- Alviggi MG
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- Ambler A
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- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
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- An F
- Anastopoulos C
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- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
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- Asimakopoulou EM
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- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
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- Bocci A
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- Budagov IA
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- Buschmann E
- Bussey PJ
- Butler JM
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- Buttinger W
- Buzatu A
- Buzykaev AR
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- Cabras G
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- Caforio D
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- Cairo VMM
- Cakir IT
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- Calace N
- Calafiura P
- Calandri A
- Calderini G
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- Calvet D
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- Carli I
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- Casha AF
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- Castillo FL
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- Chargeishvili B
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- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
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- Ciocio A
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- de Renstrom PAB
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- Iconomidou-Fayard L
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- Ikegami Y
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- Infante CMV
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- Kamenshchikov A
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- Kano Y
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- Kanzaki J
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- Karentzos E
- Karpov SN
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- Karyukhin AN
- Kashif L
- Kass RD
- Kastanas A
- Kataoka Y
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- Keeler R
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- Khandoga M
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- Khoda EE
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- Kivernyk O
- Kladiva E
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- Klein U
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- Klimek P
- Klimentov A
- Klingl T
- Klioutchnikova T
- Klitzner FF
- Kluit P
- Kluth S
- Kneringer E
- Knoops EBFG
- Knue A
- Kobayashi D
- Kobayashi T
- Kobel M
- Kocian M
- Kodys P
- Koeneke K
- Koenig PT
- Koffas T
- Koi T
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- Koletsou I
- Komarek T
- Kondo T
- Kondrashova N
- Konig AC
- Kono T
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- Konya B
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- Korolkova E
- Korotkova N
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- Kosek T
- Kostyukhin VV
- Kotwal A
- Koulouris A
- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kourlitis E
- Kouskoura V
- Kowalewska AB
- Kowalewski R
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- Kozanecki W
- Kozhin AS
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- Krauss D
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- Kukla R
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- Kuleshov S
- Kulinich YP
- Kuna M
- Kunigo T
- Kupco A
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- Kuprash O
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- Kurova A
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- Lanza A
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- Laplace S
- Laporte JF
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- Latour BMD
- Lau TS
- Laudrain A
- Laurier A
- Lavorgna M
- Lazzaroni M
- Le Dortz O
- Le Guirriec E
- Le B
- LeBlanc M
- LeCompte T
- Ledroit-Guillon F
- Lee CA
- Lee GR
- Lee L
- Lee SC
- Lee SJ
- Lefebvre B
- Lefebvre M
- Legger F
- Leggett C
- Lehmann K
- Lehmann N
- Leight WA
- Leisos A
- Leite MAL
- Leitgeb CE
- Leitner R
- Lellouch D
- Leney KJC
- Lenz T
- Lenzi B
- Leone R
- Leone S
- Leonidopoulos C
- Leopold A
- Lerner G
- Leroy C
- Les R
- Lester CG
- Levchenko M
- Levin D
- Levinson LJ
- Levque J
- Lewis DJ
- Li B
- Li C-Q
- Li F
- Li H
- Li J
- Li K
- Li L
- Li M
- Li Q
- Li QY
- Li S
- Li X
- Li Y
- Li Z
- Liang Z
- Liberti B
- Liblong A
- Lie K
- Liem S
- Lin CY
- Lin K
- Lin TH
- Linck RA
- Lindon JH
- Lionti AL
- Lipeles E
- Lipniacka A
- Lisovyi M
- Liss TM
- Lister A
- Litke AM
- Little JD
- Liu B
- Liu BL
- Liu H
- Liu HB
- Liu JB
- Liu JKK
- Liu K
- Liu M
- Liu P
- Liu Y
- Liu YL
- Liu YW
- Livan M
- Llacer MM
- Lleres A
- Lloyd SL
- Lo Sterzo F
- Lo CY
- Lobodzinska EM
- Loch P
- Loesel PJ
- Loesle A
- Loffredo S
- Lohse T
- Lohwasser K
- Lokajicek M
- Long JD
- Long RE
- Longo L
- Looper KA
- Lopez JA
- Lorenz J
- Losada M
- Lou X
- Lounis A
- Love J
- Love PA
- Lozano Bahilo JJ
- Lu M
- Lu YJ
- Lubatti HJ
- Luci C
- Lucotte A
- Luedtke C
- Luehring F
- Luise I
- Luminari L
- Lund-Jensen B
- Lutz MS
- Lynn D
- Lysak R
- Lytken E
- Lyu F
- Lyubushkin V
- Lyubushkina T
- Ma H
- Ma LL
- Ma Y
- Maccarrone G
- Macchiolo A
- Macdonald CM
- Macek B
- Madaffari D
- Madar R
- Madden WDB
- Mader WF
- Madysa N
- Maeda J
- Maekawa K
- Maeland S
- Maeno T
- Maerker M
- Maettig P
- Maevskiy AS
- Magerl V
- Magini N
- Mahon DJ
- Maidantchik C
- Maier T
- Maio A
- Maira NV
- Majersky O
- Majewski S
- Makida Y
- Makovec N
- Malaescu B
- Malecki P
- Maleev VP
- Malek F
- Mallik U
- Malon D
- Malone C
- Maltezos S
- Malyukov S
- Mamuzic J
- Mancini G
- Mandi IC
- Manghi FL
- Manhaes de Andrade Filho L
- Maniatis IM
- Mankinen KH
- Mann A
- Manousos A
- Mansoulie B
- Manthos I
- Manzoni S
- Marantis A
- Marceca G
- Marchese L
- Marchiori G
- Marcisovsky M
- Marcon C
- Marjanovic M
- Marroquim F
- Marshall Z
- Martensson MUF
- Marti-Garcia S
- Martin CB
- Martin TA
- Martin VJ
- Martin-Haugh S
- Martinelli L
- Martinez M
- Martinez NL
- Martoiu VS
- Martyniuk AC
- Marzin A
- Maschek SR
- Masetti L
- Mashimo T
- Mashinistov R
- Masik J
- Maslennikov AL
- Mason LH
- Massa L
- Massarotti P
- Mastrandrea P
- Mastroberardino A
- Masubuchi T
- Matic A
- Maurer J
- Maxfield SJ
- Maximov DA
- Mazini R
- Maznas I
- Mazza SM
- Mc Kee SP
- McCarthy TG
- McClymont L
- McCormack WP
- McDonald EF
- Mcfayden JA
- McKay MA
- McLean KD
- McMahon SJ
- McNamara PC
- McNicol CJ
- McPherson RA
- Mdhluli JE
- Meadows ZA
- Meehan S
- Megy T
- Mehlhase S
- Mehta A
- Meideck T
- Meirose B
- Melini D
- Mellado Garcia BR
- Mellenthin JD
- Melo M
- Meloni F
- Melzer A
- Menary SB
- Mendes Gouveia ED
- Meng L
- Meng XT
- Menke S
- Meoni E
- Mergelmeyer S
- Merino JL
- Merkt SAM
- Merlassino C
- Mermod P
- Merola L
- Meroni C
- Meshkov O
- Meshreki JKR
- Messina A
- Metcalfe J
- Mete AS
- Meyer C
- Meyer J
- Meyer J-P
- Miano F
- Middleton RP
- Miguens JM
- Mijovic L
- Mikenberg G
- Mikestikova M
- Mikuz M
- Mildner H
- Milesi M
- Milic A
- Millar DA
- Miller DW
- Milosavljevic MV
- Milov A
- Milstead DA
- Mina RA
- Minaenko AA
- Minano Moya M
- Minashvili IA
- Mincer A
- Mindur B
- Mineev M
- Minegishi Y
- Ming Y
- Miotto GL
- Mir LM
- Mirto A
- Mistry KP
- Mitani T
- Mitrevski J
- Mitsou VA
- Mittal M
- Miucci A
- Miyagawa PS
- Mizukami A
- Mjornmark JU
- Mkrtchyan T
- Mlynarikova M
- Moa T
- Mochizuki K
- Moenig K
- Mogg P
- Mohamed ATA
- Mohapatra S
- Moles-Valls R
- Mondragon MC
- Monk J
- Monnier E
- Montalbano A
- Montella M
- Monticelli F
- Monzani S
- Morales AR
- Morales FAJ
- Morange N
- Moreno Martinez C
- Moreno D
- Morettini P
- Morgenstern M
- Morgenstern S
- Mori D
- Morii M
- Morinaga M
- Morisbak V
- Morley AK
- Mornacchi G
- Morris AP
- Morvaj L
- Moschovakos P
- Moser B
- Mosidze M
- Moskalets T
- Moss HJ
- Moss J
- Motohashi K
- Mountricha E
- Moyse EJW
- Muanza S
- Mueller J
- Mueller RSP
- Muenstermann D
- Mullier GA
- Munoz Martinez JL
- Murin P
- Murray WJ
- Murrone A
- Muskinja M
- Mwewa C
- Myagkov AG
- Myers J
- Myska M
- Nachman BP
- Nackenhorst O
- Nag AN
- Nagai K
- Nagano K
- Nagasaka Y
- Nagel M
- Nagy E
- Nairz AM
- Nakahama Y
- Nakamura K
- Nakamura T
- Nakano I
- Nanjo H
- Napolitano F
- Narayan R
- Naryshkin I
- Naumann T
- Navarro G
- Neal HA
- Nechaeva PY
- Nechansky F
- Neep TJ
- Negri A
- Negrini M
- Nellist C
- Nelson ME
- Nemecek S
- Nemethy P
- Nessi M
- Neubauer MS
- Neumann M
- Newman PR
- Ng TY
- Ng YS
- Ng YWY
- Nguyen Manh T
- Nguyen HDN
- Nibigira E
- Nickerson RB
- Nicolaidou R
- Nielsen DS
- Nielsen J
- Nikiforou N
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsson P
- Nindhito HR
- Ninomiya Y
- Nisati A
- Nishu N
- Nisius R
- Nitsche I
- Nitta T
- Nobe T
- Noguchi Y
- Nomidis I
- Nomura MA
- Nordberg M
- Norjoharuddeen N
- Novak T
- Novgorodova O
- Novotny R
- Nozka L
- Ntekas K
- Nurse E
- O'Connor K
- O'Neil DC
- Oakham FG
- Oberlack H
- Ocariz J
- Ochi A
- Ochoa I
- Ochoa-Ricoux JP
- Oda S
- Odaka S
- Oerdek S
- Ogrodnik A
- Oh A
- Oh SH
- Ohm CC
- Oide H
- Ojeda ML
- Okawa H
- Okazaki Y
- Okumura Y
- Okuyama T
- Olariu A
- Oleiro Seabra LF
- Olivares Pino SA
- Oliver JL
- Olsson MJR
- Olszewski A
- Olszowska J
- Onofre A
- Onogi K
- Onyisi PUE
- Oppen H
- Oreglia MJ
- Orellana GE
- Oren Y
- Orestano D
- Orlando N
- Orr RS
- OShea V
- Ospanov R
- Otero y Garzon G
- Otono H
- Ouchrif M
- Ouellette J
- Ould-Saada F
- Ouraou A
- Outschoorn VIM
- Ouyang Q
- Owen M
- Owen RE
- Ozcan VE
- Ozturk N
- Pacalt J
- Pacey HA
- Pachal K
- Pacheco Pages A
- Padilla Aranda C
- Paganini M
- Palacino G
- Palazzo S
- Palestini S
- Palka M
- Pallin D
- Panagoulias I
- Pandini CE
- Pani P
- Panizzo G
- Paolozzi L
- Papadatos C
- Papageorgiou K
- Paramonov A
- Parida B
- Park TH
- Parker AJ
- Parker MA
- Parodi F
- Parrish EWP
- Parsons JA
- Parzefall U
- Pascual JAG
- Pascuzzi VR
- Pasner JMP
- Pasqualucci E
- Passaggio S
- Pastor ET
- Pastore F
- Pasuwan P
- Pataraia S
- Pater JR
- Pathak A
- Pauly T
- Paz IL
- Pearson B
- Pedersen M
- Pedro R
- Peiffer T
- Peleganchuk S
- Pena JJ
- Penc O
- Peng H
- Peralva BS
- Perego MM
- Pereira Peixoto AP
- Perepelitsa D
- Perez MV
- Peri F
- Perini L
- Pernegger H
- Perrella S
- Peters K
- Peters RFY
- Petersen BA
- Petersen TC
- Petit E
- Petridis A
- Petridou C
- Petroff P
- Petrov M
- Petrucci F
- Pettee M
- Pettersson NE
- Petukhova K
- Peyaud A
- Pezoa R
- Pezzotti L
- Pham T
- Phillips FH
- Phillips PW
- Phipps MW
- Piacquadio G
- Pianori E
- Picazio A
- Pickles RH
- Piegaia R
- Pietreanu D
- Pilcher JE
- Pilkington AD
- Pinamonti M
- Pineda AS
- Pinfold JL
- Pinto MVB
- Pitt M
- Pizzimento L
- Pleier M-A
- Pleskot V
- Plotnikova E
- Pluth D
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pogrebnyak I
- Pohl D
- Pokharel I
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Ponomarenko D
- Pontecorvo L
- Popa S
- Popeneciu GA
- Pospisil S
- Potamianos K
- Potrap IN
- Potter CJ
- Potti H
- Poulsen T
- Poveda J
- Powell TD
- Pownall G
- Pralavorio P
- Prell S
- Price D
- Primavera M
- Prince S
- Proffitt ML
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
- Pudzha D
- Puri A
- Puzo P
- Qian J
- Qin Y
- Quadt A
- Queitsch-Maitland M
- Quintero DMP
- Qureshi A
- Rados P
- Ragusa F
- Rahal G
- Raine JA
- Rajagopalan S
- Ramos JM
- Ran K
- Rashid T
- Raspopov S
- Ratti MG
- Rauch DM
- Rauscher F
- Rave S
- Ravina B
- Ravinovich I
- Rawling JH
- Raymond M
- Read AL
- Readioff NP
- Reale M
- Rebuzzi DM
- Redelbach A
- Redlinger G
- Reeves K
- Rehnisch L
- Reichert J
- Reikher D
- Reiss A
- Rej A
- Rembser C
- Renda M
- Renous DS
- Rescigno M
- Resconi S
- Resseguie ED
- Rettie S
- Reynolds E
- Rezanova OL
- Reznicek P
- Rhr F
- Ricci E
- Richter R
- Richter S
- Richter-Was E
- Ricken O
- Ridel M
- Rieck P
- Riegel CJ
- Rifki O
- Rijssenbeek M
- Rimoldi A
- Rimoldi M
- Rinaldi L
- Ripellino G
- Risti BC
- Ritsch E
- Riu I
- Rizatdinova F
- Rizvi E
- Rizzi C
- Roberts RT
- Robertson SH
- Robin M
- Robinson D
- Robinson JEM
- Robles Gajardo CM
- Robson A
- Rocco E
- Roda C
- Rodriguez Bosca S
- Rodriguez Perez A
- Rodriguez Rodriguez D
- Roe S
- Roehrig R
- Rohne O
- Roland CPA
- Roloff J
- Romaniouk A
- Romano M
- Rompotis N
- Ronzani M
- Roos L
- Rosati S
- Rosbach K
- Rosin G
- Rosser BJ
- Rossi E
- Rossi LP
- Rossini L
- Rosten R
- Rotaru M
- Rothberg J
- Rousseau D
- Rovelli G
- Roy D
- Rozanov A
- Rozen Y
- Ruan X
- Rubbo F
- Ruettinger EM
- Ruiz-Martinez A
- Rummler A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rustige L
- Rutherfoord JP
- Ryabov YF
- Rybar M
- Rybkin G
- Ryzhov A
- Rzehorz GF
- Sabatini P
- Sabato G
- Sacerdoti S
- Sadrozinski HF-W
- Sadykov R
- Saenz SRP
- Saha P
- Saha S
- Sahinsoy M
- Sahu A
- Saimpert M
- Saito M
- Saito T
- Sakamoto H
- Sakharov A
- Salamani D
- Salamanna G
- Salazar Loyola JE
- Salihagic D
- Salnikov A
- Salt J
- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
- Samani BS
- Samarati J
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez CAS
- Sanchez FJM
- Sanchez J
- Sandaker H
- Sander CO
- Sanderswood IG
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sano Y
- Sansoni A
- Santoni C
- Santos H
- Santpur SN
- Santra A
- Santurio EV
- Sapronov A
- Saraiva JG
- Sasaki O
- Sato K
- Sauvan E
- Savard P
- Savic N
- Sawada R
- Sawyer C
- Sawyer L
- Sbarra C
- Sbrizzi A
- Scanlon T
- Schaarschmidt J
- Schacht P
- Schachtner BM
- Schaefer D
- Schaefer L
- Schaeffer J
- Schaepe S
- Schaffer AC
- Schaile D
- Schamberger RD
- Scharmberg N
- Schegelsky VA
- Scheirich D
- Schenck F
- Schernau M
- Schfer U
- Schiavi C
- Schier S
- Schildgen LK
- Schillaci ZM
- Schioppa EJ
- Schioppa M
- Schleicher KE
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schmoeckel JC
- Schnoor U
- Schoeffel L
- Schoening A
- Scholer PG
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder F
- Schroeder TV
- Schulte A
- Schultz-Coulon H-C
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scodeggio M
- Scornajenghi M
- Scuri F
- Scutti F
- Scyboz LM
- Sebastiani CD
- Seema P
- Seidel SC
- Seiden A
- Seiss T
- Seixas JM
- Sekhniaidze G
- Sekhon K
- Sekula SJ
- Semprini-Cesari N
- Sen S
- Senkin S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shahinian JD
- Shaikh NW
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Sharma A
- Sharma AS
- Shatalov PB
- Shaw K
- Shaw SM
- Shcherbakova A
- Shen Y
- Sherafati N
- Sherman AD
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimogama Y
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet MJ
- Shojaii S
- Shope DR
- Shrestha S
- Shulga E
- Sicho P
- Sickles AM
- Sidebo PE
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva Oliveira M
- Silva M
- Silverstein SB
- Simion S
- Simioni E
- Simoniello R
- Simsek S
- Sinervo P
- Sinev NB
- Sioli M
- Siral I
- Sivoklokov SY
- Sjolin J
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smizanska M
- Smolek K
- Smykiewicz A
- Snesarev AA
- Snoek HL
- Snyder IM
- Snyder S
- Sobie R
- Soffa AM
- Soffer A
- Sogaard A
- Sohns F
- Sola JDB
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov O
- Solovyev V
- Sommer P
- Son H
- Song W
- Song WY
- Sopczak A
- Sopkova F
- Sotiropoulou CL
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Spagnolo S
- Spalla M
- Span F
- Spangenberg M
- Sperlich D
- Spieker TM
- Spighi R
- Spigo G
- Spina M
- Spiteri DP
- Spousta M
- Stabile A
- Stamas BL
- Stamen R
- Stamenkovic M
- Stanecka E
- Stanek RW
- Stanislaus B
- Stanitzki MM
- Stankaityte M
- Stapf B
- Starchenko EA
- Stark GH
- Stark J
- Stark SH
- Staroba P
- Starovoitov P
- Staszewski R
- Stavropoulos G
- Stegler M
- Steinberg P
- Steinhebel AL
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stevenson TJ
- Stewart GA
- Stockton MC
- Stoicea G
- Stolarski M
- Stolte P
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Straz S
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
- Suchek S
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Takai H
- Takashima R
- Takeda K
- Takeshita T
- Takeva EP
- Takubo Y
- Talby M
- Talyshev AA
- Tamir NM
- Tanaka J
- Tanaka M
- Tanaka R
- Tapprogge S
- Tarem S
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor AJ
- Taylor GN
- Taylor W
- Tee AS
- Tehrani FS
- Teixeira-Dias P
- Ten Kate H
- Teoh JJ
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Thais SJ
- Theveneaux-Pelzer T
- Thiele F
- Thomas DW
- Thomas JO
- Thomas JP
- Thompson AS
- Thompson PD
- Thomsen LA
- Thomson E
- Tian Y
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Tobon CAM
- Todome K
- Todorova-Nova S
- Todt S
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
- Tomiwa KG
- Tomoto M
- Tompkins L
- Toms K
- Tong B
- Tornambe P
- Toro RC
- Torrence E
- Torres H
- Torres RET
- Tosciri C
- Toth J
- Tovey DR
- Traeet A
- Treado CJ
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trovatelli M
- Trovato F
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tseng JC-L
- Tsiareshka P
- Tsirigotis A
- Tsirintanis N
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
- Turner RJ
- Turra RT
- Tuts PM
- Tzamarias S
- Tzovara E
- Ucchielli G
- Uchida K
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Urban J
- Urquijo P
- Usai G
- Usui J
- Uysal Z
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Valls Ferrer JA
- Van Daalen TR
- Van Gemmeren P
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vaniachine A
- Vannicola D
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez Furelos D
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi N
- Vera AMR
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vetterli MC
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Villar DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
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- Wagner-Kuhr J
- Wahlberg H
- Wakamiya K
- Walbrecht VM
- Walder J
- Walker R
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- Wallangen V
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- Washbrook A
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- Whalen K
- Whallon NL
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- Whiteson D
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- Wickens FJ
- Wiedenmann W
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- Wilkins LJ
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- Winter BT
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- Yajima K
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- Yamamoto A
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- Yamatani M
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- Yao W-M
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- Yasu Y
- Yatsenko E
- Ye J
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- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Yuen SPY
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang DF
- Zhang F
- Zhang G
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- Zhang J
- Zhang L
- Zhang M
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- Zhao P
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- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou MS
- Zhou N
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- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2019
- Field of study
The inclusive cross-section for jet production in association with a Z boson decaying into an electron–positron pair is measured as a function of the transverse momentum and the absolute rapidity of jets using 19.9 fb −1 of s√=8 TeV proton–proton collision data collected with the ATLAS detector at the Large Hadron Collider. The measured Z + jets cross-section is unfolded to the particle level. The cross-section is compared with state-of-the-art Standard Model calculations, including the next-to-leading-order and next-to-next-to-leading-order perturbative QCD calculations, corrected for non-perturbative and QED radiation effects. The results of the measurements cover final-state jets with transverse momenta up to 1 TeV, and show good agreement with fixed-order calculations
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