495 research outputs found
A fitness assay for comparing RNAi effects across multiple C. elegans genotypes
- Author
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>RNAi technology by feeding of <it>E. coli </it>containing dsRNA in <it>C. elegans </it>has significantly contributed to further our understanding of many different fields, including genetics, molecular biology, developmental biology and functional genomics. Most of this research has been carried out in a single genotype or genetic background. However, RNAi effects in one genotype do not reveal the allelic effects that segregate in natural populations and contribute to phenotypic variation.</p> <p>Results</p> <p>Here we present a method that allows for rapidly comparing RNAi effects among diverse genotypes at an improved high throughput rate. It is based on assessing the fitness of a population of worms by measuring the rate at which <it>E. coli </it>is consumed. Critically, we demonstrate the analytical power of this method by QTL mapping the loss of RNAi sensitivity (in the germline) in a recombinant inbred population derived from a cross between Bristol and a natural isolate from Hawaii. Hawaii has lost RNAi sensitivity in the germline. We found that polymorphisms in <it>ppw-1 </it>contribute to this loss of RNAi sensitivity, but that other loci are also likely to be important.</p> <p>Conclusions</p> <p>In summary, we have established a fast method that improves the throughput of RNAi in liquid, that generates quantitative data, that is easy to implement in most laboratories, and importantly that enables QTL mapping using RNAi.</p
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
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- Varnes EW
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- Vukotic I
- Wagner P
- Wagner W
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- Wahdan S
- Wahlberg H
- Walbrecht VM
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- Whitmore BW
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- Winkels E
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- Wong VWS
- Woods NL
- Worm SD
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- Wozniak KW
- Wraight K
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- Xella S
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- Yallup DP
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- Yamamoto A
- Yamatani M
- Yamazaki T
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- Yao W-M
- Yap YC
- Yasu Y
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- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
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- Zahreddine J
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- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- 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
- 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
A mRNA landscape of bovine embryos after standard and MAPK-inhibited culture conditions: a comparative analysis.
- Author
- A Graf
- A Ralston
- AC Eklund
- AC Nicacio
- AV Zimin
- B Plusa
- B Wilkinson
- Bas Brinkhof
- Bernard AJ Roelen
- BPVL Telugu
- C Chazaud
- D Acampora
- D Rizos
- D Strumpf
- D Xie
- DA Stringfellow
- DK Berg
- DR Khan
- EW Kuijk
- F Izadyar
- Frank M Riemers
- GA Bó
- GR Martin
- H Auer
- H Nagatomo
- H Sumer
- H Wu
- Helena TA van Tol
- Henk P Haagsman
- J Nichols
- J SantaLucia
- J Schindelin
- JA Hackett
- JA Thomson
- JA Thomson
- JH Kim
- JJ Parrish
- JM Veltmaat
- JS Kuo
- K Imakawa
- K Kondoh
- K Kurimoto
- Kaveh Mashayekhi
- KM Johnson
- KM Loh
- L Brown
- L Shi
- LA Boyer
- LS Lim
- M Buehr
- M Fürthauer
- M Ozawa
- M Roode
- M Van Der Jeught
- M Yamaji
- M Zernicka-Goetz
- M Zuker
- MA Sirard
- Marian JA Groot Koerkamp
- MC Wallingford
- MJ Evans
- N Grabole
- N Schrode
- NB Ivanova
- P Roepman
- Q Li
- Q Ying
- QL Ying
- R Edgar
- R Jaenisch
- RM Roberts
- S Kurosaka
- S Tanaka
- S Wageningen van
- Sascha G IJzer
- SH Yang
- SJ Roper
- T Casci
- T Ezashi
- T Hamatani
- T Margaritis
- T Sakaguchi
- T Sakurai
- TS Tanaka
- WA Kues
- WN D’Souza
- Y Chu
- Y Grinblat
- Y Wang
- Y Yamanaka
- YH Loh
- YH Yang
- Z Du
- Z Ma
- Z Madeja
- Z Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
BACKGROUND: Genes and signalling pathways involved in pluripotency have been studied extensively in mouse and human pre-implantation embryos and embryonic stem (ES) cells. The unsuccessful attempts to generate ES cell lines from other species including cattle suggests that other genes and pathways are involved in maintaining pluripotency in these species. To investigate which genes are involved in bovine pluripotency, expression profiles were generated from morula, blastocyst, trophectoderm and inner cell mass (ICM) samples using microarray analysis. As MAPK inhibition can increase the NANOG/GATA6 ratio in the inner cell mass, additionally blastocysts were cultured in the presence of a MAPK inhibitor and changes in gene expression in the inner cell mass were analysed. RESULTS: Between morula and blastocyst 3,774 genes were differentially expressed and the largest differences were found in blastocyst up-regulated genes. Gene ontology (GO) analysis shows lipid metabolic process as the term most enriched with genes expressed at higher levels in blastocysts. Genes with higher expression levels in morulae were enriched in the RNA processing GO term. Of the 497 differentially expressed genes comparing ICM and TE, the expression of NANOG, SOX2 and POU5F1 was increased in the ICM confirming their evolutionary preserved role in pluripotency. Several genes implicated to be involved in differentiation or fate determination were also expressed at higher levels in the ICM. Genes expressed at higher levels in the ICM were enriched in the RNA splicing and regulation of gene expression GO term. Although NANOG expression was elevated upon MAPK inhibition, SOX2 and POU5F1 expression showed little increase. Expression of other genes in the MAPK pathway including DUSP4 and SPRY4, or influenced by MAPK inhibition such as IFNT, was down-regulated. CONCLUSION: The data obtained from the microarray studies provide further insight in gene expression during bovine embryonic development. They show an expression profile in pluripotent cells that indicates a pluripotent, epiblast-like state. The inability to culture ICM cells as stem cells in the presence of an inhibitor of MAPK activity together with the reported data indicates that MAPK inhibition alone is not sufficient to maintain a pluripotent character in bovine cells
Brazilian Consensus on Photoprotection
- Author
- Abarca J
- Abdel-Malek Z
- Abel E
- Acosta LR
- Adam J
- Ahmed AM
- Alaluf S
- Almutawa F
- Aloai JF
- Aloia JF
- Aloia JF
- Alonso-Lebrero JL
- Alves LM
- Anderson RR
- Andersson-Willman B
- Andrés-Lacueva C
- Aripuanã Cobério Terena
- Armstrong AW
- Avenel-Audran M
- Avenel-Audran M
- Bachrach S
- Bais AF
- Balk SJ
- Balk SJ
- Ball Arefiev KL
- Balogh TS
- Batista T
- Battie C
- Bauer A
- Bauer J
- Baumann L
- Bech-Thomsen N
- Becker JA
- Benvenuto-Andrade C
- Berneburg M
- Bernstein EF
- Biesalski HK
- Binkley N
- Binkley N
- Bischoff-Ferrari HA
- Bodekaer M
- Boisen AM
- Bouilly-Gauthier D
- Boyd AS
- Bradford PT
- Broekmans WM
- Bucay VW
- Buendía Eisman A
- Buendía-Eisman A
- Buller DB
- Buller DB
- Caccialanza M
- Camera E
- Capote R
- Carolina Reato Marçon
- Castanedo-Cazares JP
- Cestari T
- Chan AC
- Chen AC
- Chen L
- Chen T
- Chesney RW
- Chiu YE
- Cho HS
- Cho S
- Clemens TL
- Corrêa MP
- Corrêa MP
- Corrêa MP
- Costa FB
- Crane LA
- Crane LA
- Criado P
- Cross SE
- Cusack C
- D'Orazio J
- Dain SJ
- Darlington S
- Darvin ME
- Dattani JT
- Davis A
- Day AK
- de Gruijl FR
- de Laat A
- de Paula Corrêa M
- de Paula Corrêa M
- de Paula Corrêa M
- Denise Steiner
- Dennis LK
- Diffey BL
- Diffey BL
- Diffey BL
- Diffey BL
- Dlugos DJ
- Dobs AS
- Dominguez AR
- Draelos ZD
- Draelos ZD
- Draelos ZD
- Draelos ZD
- Duarte I
- Dumay O
- Dunnigan MG
- Dusza SW
- Eadie E
- Eberlein-König B
- Edwards Jr EK
- Eicker J
- Eloisa Leis Ayres
- Engelsen O
- English DR
- Erden Inal M
- Erden Inal M
- Fabris MR
- Falk M
- Farrerons J
- Farrerons J
- Fartasch M
- Fioletov VE
- Fitzpatrick TB
- Flávia Alvim Sant'anna Addor
- Flávia Naranjo Ravelli
- Fonseca V
- Fryer MJ
- Fuller R
- Gambichler T
- Gambichler T
- Garcia F
- Gaspar LR
- Geller AC
- Ghazi S
- Gies P
- Gilaberte Y
- Gilchrest BA
- Ginde AA
- Glanz K
- Glanz K
- Glanz K
- Glass D
- Glazebrook C
- Glazer JL
- Godar DE
- Godar DE
- Gonzales S
- Gonzalez S
- Gonzalez S
- Grant WB
- Greul AK
- Groves GA
- Grune T
- Guevara IL
- Guinot C
- Gupta AK
- Guéniche A
- Guéniche A
- Hackenberg S
- Halder RM
- Halliwell B
- Haluza D
- Harms J
- Harris SS
- Hatch KL
- Hatua P
- Haywood R
- Heinrich U
- Helio Amante Miot
- Hercogova J
- Hexsel CL
- Heydenreich J
- Higuera-Ciapara I
- Hillhouse J
- Hodgkin P
- Holick MF
- Holick MF
- Holick MF
- Holick MF
- Holick MF
- Hollis BW
- Holloway L
- Hougaard KS
- Humberto Ponzio
- Hussein MR
- Hönigsmann H
- Ida Duarte
- Inamadar AC
- Isedeh P
- Jane Neffá
- Jennings L
- Jeon HY
- José Antônio Jabur da Cunha
- Jou PC
- Juliana Catucci Boza
- Jung GW
- Jung GW
- Jung T
- Kamen DL
- Kanofsky JR
- Kasichayanula S
- Katiyar SK
- Katiyar SK
- Kaur IP
- Kein RS
- Kennedy Carney C
- Kenneth K
- Kerzendorfer C
- Khadir K
- Khavkin J
- Kibbe AH
- Kim SS
- Kimlin M
- Kimlin MG
- Klein GL
- Klein GL
- Klein GL
- Klein RS
- Kligman EW
- Kniess CT
- Koch H
- Koeneman BA
- Koh HK
- Koshy JC
- Kraft JN
- Krutmann J
- Krutmann J
- Krämer M
- Kullavanijava P
- Kullavanijaya P
- Kullavanijya P
- Kyle JW
- Köpcke W
- Kütting B
- Lagerlund M
- Lakhdar H
- Lambert JD
- Lambert R
- Lautenschlager S
- Lee EH
- Lee HS
- Lee J
- Lester E
- Lin JS
- Lin JY
- Liu PT
- Lo CW
- Loden M
- Lodén M
- Looker AC
- Lorenz RT
- Lotti T
- Lowe NJ
- Lu Z
- Lucci A
- Lucena EE
- Luciana de Paula Samorano
- Lyons NM
- MacLaughlin J
- MacLaughlin JA
- MacNeal RJ
- Madronich S
- Mahler HI
- Mahmoud BH
- Mahmoud BH
- Mahmoud BH
- Maia M
- Maier H
- Maillan P
- Makrantonaki E
- Malabanan A
- Malvy DJ
- Manach C
- Manicourt DH
- Mansur JS
- Marcelo de Paula Corrêa
- Marcus Maia
- Marks R
- Massagué J
- Massenkeil G
- Mathews-Roth MM
- Matsui MS
- Matsumura Y
- Matsuoka LY
- Matsuoka LY
- Matsuoka LY
- Matsuoka LY
- Melia J
- Metry DW
- Middelkamp-Hup MA
- Middelkamp-Hup MA
- Mills A
- Mireles-Rocha H
- Moehrle M
- Moehrle M
- Montagnani M
- Monteiro EO
- Morganti P
- Morison WL
- Morison WL
- Moskaug JØ
- Moyal D
- Moyal D
- Moyal D
- Murphy GM
- Murphy GM
- Murphy ME
- Naylor MF
- Need AG
- Ni Z
- Nichols JA
- Nichols K
- Nilton Nasser
- Nordlund JJ
- Norman GJ
- Norsang G
- Norval M
- O'Donoghue MN
- O'Riordan JL
- Olga Maria Rodrigues Ribeiro Leite
- Olsen EA
- Orentreich D
- Osterwalder U
- Otávio Sergio Lopes
- Palm M
- Palombo P
- Parisi AV
- Parisi AV
- Parrish JA
- Paterson CR
- Pedro Dantas Oliveira
- Peguet-Navarro J
- Petit-Frère C
- Pfeifer MT
- Pichardo R
- Pichon LC
- Pillai S
- Pinnell SR
- Placzek M
- Polefka TG
- Pollack RJ
- Preece MA
- Prista LN
- Prochaska JO
- Prochaska JO
- Pujol JA
- Purim K
- Purim KS
- Pustisek N
- Pérez-Castrillón JL
- Quan T
- Quatrano NA
- Querings K
- Querings K
- Rabe JH
- Ragi JM
- Ramasubramaniam R
- Ray AJ
- Reeder AI
- Reichrath J
- Rejnmark L
- Renata Leal Bregunci Meyer
- Rendon M
- Reynolds KD
- Rhodes LE
- Ribaya-Mercado JD
- Rigel DS
- Rittié L
- Roelandts R
- Rona C
- Ross AC
- Rudolf M
- Salih FM
- Saliou C
- Sambandan DR
- Saraiya M
- Sayre RM
- Sayre RM
- Scalbert A
- Scalbert A
- Scarmo S
- Schagen SK
- Schalka S
- Schalka S
- Schalka S
- Schauder S
- Scheuer E
- Schieke SM
- Schieke SM
- Schlossman D
- Schlumpf M
- Schneider S
- Schroeder P
- Schwarz A
- Schwarz A
- Sedrani SH
- Segal E
- Seite S
- Seité S
- Seité S
- Shaat NA
- Shaath N
- Sheehan JM
- Sheth VM
- Shuster S
- Sies H
- Sies H
- Signori V
- Silva A
- Silva A
- Sklar LR
- Sklar LR
- Sliney DH
- Sollitto RB
- Stahl W
- Stahl W
- Stanfield JW
- Stapleton J
- Stechschulte SA
- Stender IM
- Stengel FM
- Stengel FM
- Stern RS
- Stoebner-Delbarre A
- Suganuma K
- Suh KS
- Summers P
- Suppa M
- Svobodova A
- Swerdlow AJ
- Sérgio Schalka
- Tan JK
- Tatiana Steiner
- Teixeira SMMCG
- Teixeira SP
- Teulings HE
- Thieden E
- Thieden E
- Thomas K
- Thompson SC
- Tjellesen L
- Townsend JS
- Trueb RM
- Tuchinda C
- Tuchinda C
- Turnbull DJ
- Turrisi R
- Tânia Cestari
- Umezawa M
- Urasaki MBM
- Vachiramon V
- Vainio H
- van Dijk A
- Victor FC
- Vieth R
- Vitor Manoel Silva dos Reis
- Vitória Regina Pedreira de Almeida Rego
- Vázquez M
- Walder BK
- Walker SL
- Wang SQ
- Wang SQ
- Wang SQ
- Waterston K
- Watson RE
- Webb AR
- Webb AR
- Webb AR
- Webb AR
- Wei H
- Weisman Y
- Wesson KM
- Wexler RK
- Wilkinson RJ
- Williams S
- Wolf C
- Wolf R
- Wu Y
- Wysong A
- Yaar M
- Yashiro K
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- 01/01/2014
- Field of study
Brazil is a country of continental dimensions with a large heterogeneity of climates and massive mixing of the population. Almost the entire national territory is located between the Equator and the Tropic of Capricorn, and the Earth axial tilt to the south certainly makes Brazil one of the countries of the world with greater extent of land in proximity to the sun. The Brazilian coastline, where most of its population lives, is more than 8,500 km long. Due to geographic characteristics and cultural trends, Brazilians are among the peoples with the highest annual exposure to the sun. Epidemiological data show a continuing increase in the incidence of nonmelanoma and melanoma skin cancers. Photoprotection can be understood as a set of measures aimed at reducing sun exposure and at preventing the development of acute and chronic actinic damage. Due to the peculiarities of Brazilian territory and culture, it would not be advisable to replicate the concepts of photoprotection from other developed countries, places with completely different climates and populations. Thus the Brazilian Society of Dermatology has developed the Brazilian Consensus on Photoprotection, the first official document on photoprotection developed in Brazil for Brazilians, with recommendations on matters involving photoprotection
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
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- Alberghi GL
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- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
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- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhou Y
- Zhu CG
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
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
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Appelt C
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
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- Zhemchugov A
- Zheng Z
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- 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.]
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
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- Zhemchugov A
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- Zimine NI
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Measurement of the energy asymmetry in t(t)over-barj production at 13 TeV with the ATLAS experiment and interpretation in the SMEFT framework
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- Abbott B
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- Abhayasinghe DK
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- Yao W-M
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- Yexley MR
- Yildiz H Duran
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yuan M
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zagazeta LF Gutierrez
- Zaid E
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaplatilek O
- Zeissner S
- Zeitnitz C
- Zeng JC
- Zenger DT
- Zenin O
- Zenis T
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zivkovic L
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 28/04/2022
- Field of study
A measurement of the energy asymmetry in jet-associated top-quark pair production is presented using 139fb−1
139
fb
-
1
of data collected by the ATLAS detector at the Large Hadron Collider during pp collisions at s=13TeV
s
=
13
TeV
. The observable measures the different probability of top and antitop quarks to have the higher energy as a function of the jet scattering angle with respect to the beam axis. The energy asymmetry is measured in the semileptonic ttˉ
t
t
¯
decay channel, and the hadronically decaying top quark must have transverse momentum above 350GeV
350
GeV
. The results are corrected for detector effects to particle level in three bins of the scattering angle of the associated jet. The measurement agrees with the SM prediction at next-to-leading-order accuracy in quantum chromodynamics in all three bins. In the bin with the largest expected asymmetry, where the jet is emitted perpendicular to the beam, the energy asymmetry is measured to be −0.043±0.020
-
0.043
±
0.020
, in agreement with the SM prediction of −0.037±0.003
-
0.037
±
0.003
. Interpreting this result in the framework of the Standard Model effective field theory (SMEFT), it is shown that the energy asymmetry is sensitive to the top-quark chirality in four-quark operators and is therefore a valuable new observable in global SMEFT fits
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at √s = 7, 8 and 13 TeV
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
This paper presents an analysis at next-to-next-to-leading order in the theory of quantum chromodynamics for the determination of a new set of proton parton distribution functions using diverse measurements in pp collisions at \sqrt{s} = 7, 8 and 13 TeV, performed by the ATLAS experiment at the Large Hadron Collider, together with deep inelastic scattering data from ep collisions at the HERA collider. The ATLAS data sets considered are differential cross-section measurements of inclusive W^{±} and Z/gamma^{*} boson production, W^{±} and Z boson production in association with jets, t\bar{t} production, inclusive jet production and direct photon production. In the analysis, particular attention is paid to the correlation of systematic uncertainties within and between the various ATLAS data sets and to the impact of model, theoretical and parameterisation uncertainties. The resulting set of parton distribution functions is called ATLASpdf21
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