888 research outputs found
SDF1 in the dorsal corticospinal tract promotes CXCR4+ cell migration after spinal cord injury
- Author
- A Attar
- AJ Mothe
- BJ Bhattacharyya
- CC Chan
- D Gris
- D Rossi
- Derin Birch
- Divakar Mithal
- DP Stirling
- G Moalem
- GJ Guillemin
- H Takeuchi
- HH Hofstetter
- Hosung Jung
- I Bechmann
- J Opatz
- JC Dugas
- JE Bruni
- John A Kessler
- K Meletis
- K Reiss
- L Chi
- LL Horky
- M Joshi
- M Joshi
- M Li
- M Takahashi
- O Meucci
- PB Tran
- PB Tran
- PG Popovich
- PJ Mabon
- Q Ma
- R Shechter
- Richard J Miller
- RS Klein
- S Rossignol
- SH Chalasani
- U Graumann
- Vibhu Sahni
- Vicki M Tysseling
- Y Luo
- Y Xiang
- Y Zhu
- YR Zou
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Stromal cell-derived factor-1 (SDF1) and its major signaling receptor, CXCR4, were initially described in the immune system; however, they are also expressed in the nervous system, including the spinal cord. After spinal cord injury, the blood brain barrier is compromised, opening the way for chemokine signaling between these two systems. These experiments clarified prior contradictory findings on normal expression of SDF1 and CXCR4 as well as examined the resulting spinal cord responses resulting from this signaling.</p> <p>Methods</p> <p>These experiments examined the expression and function of SDF1 and CXCR4 in the normal and injured adult mouse spinal cord primarily using CXCR4-EGFP and SDF1-EGFP transgenic reporter mice.</p> <p>Results</p> <p>In the uninjured spinal cord, SDF1 was expressed in the dorsal corticospinal tract (dCST) as well as the meninges, whereas CXCR4 was found only in ependymal cells surrounding the central canal. After spinal cord injury (SCI), the pattern of SDF1 expression did not change rostral to the lesion but it disappeared from the degenerating dCST caudally. By contrast, CXCR4 expression changed dramatically after SCI. In addition to the CXCR4+ cells in the ependymal layer, numerous CXCR4+ cells appeared in the peripheral white matter and in the dorsal white matter localized between the dorsal corticospinal tract and the gray matter rostral to the lesion site. The non-ependymal CXCR4+ cells were found to be NG2+ and CD11b+ macrophages that presumably infiltrated through the broken blood-brain barrier. One population of macrophages appeared to be migrating towards the dCST that contains SDF1 rostral to the injury but not towards the caudal dCST in which SDF1 is no longer present. A second population of the CXCR4+ macrophages was present near the SDF1-expressing meningeal cells.</p> <p>Conclusions</p> <p>These observations suggest that attraction of CXCR4+ macrophages is part of a programmed response to injury and that modulation of the SDF1 signaling system may be important for regulating the inflammatory response after SCI.</p
Kinetic modelling of competition and depletion of shared miRNAs by competing endogenous RNAs
- Author
- A Arvey
- A Baccarini
- A Fatica
- A Franks
- A Helwak
- A Joshi
- A Loinger
- A Martirosyan
- A Martirosyan
- A Nadal
- A Raveh
- A Re
- A Riba
- A Sanchez
- A Sanchez-Mejias
- AD Bosson
- AK Leung
- AM Gurtan
- AS Flynt
- B Du
- B Obermayer
- C Bosia
- C Bosia
- C Bosia
- CW Hsu
- D Baek
- D Kim
- DP Bartel
- DP Bartel
- DP Bartel
- DT Gillespie
- E Anastasiadou
- E Berezikov
- E Koller
- E Levine
- E Levine
- FA Karreth
- G Tkacik
- H Liang
- H Teimouri
- I Alvarez-Garcia
- I Bose
- I Legnini
- J Breda
- J Das
- J Fiorentino
- J Kwon
- J Noorbakhsh
- J Tsang
- JM Franco-Zorrilla
- JM Schmiedel
- L López-Maury
- L Salmena
- L Tsimring
- M Chekulaeva
- M Figliuzzi
- M Figliuzzi
- M Gerstein
- M Jens
- M Klein
- M Mauri
- M Nitzan
- M Osella
- M Osella
- M Samoilov
- MA Gibson
- MA Valencia-Sanchez
- MS Ebert
- MS Ebert
- NG Kampen Van
- P Flondor
- P Mehta
- P Sumazin
- PB Detwiler
- PS Swain
- R Denzler
- R Denzler
- RC Brewster
- RC Friedman
- RI Gregory
- S Djuranovic
- S Grigolon
- S Guil
- S Jonas
- S Mukherji
- S Pitchiaya
- S Sass
- S Wang
- SD Chandradoss
- TB Hansen
- TR Cech
- U Ala
- U Alon
- V Siciliano
- X Lai
- X Wang
- X Yuan
- Y Liang
- Y Shimoni
- Y Tay
- Y Tay
- Y Yuan
- Publication venue
- Publication date
- 22/12/2018
- Field of study
Non-conding RNAs play a key role in the post-transcriptional regulation of
mRNA translation and turnover in eukaryotes. miRNAs, in particular, interact
with their target RNAs through protein-mediated, sequence-specific binding,
giving rise to extended and highly heterogeneous miRNA-RNA interaction
networks. Within such networks, competition to bind miRNAs can generate an
effective positive coupling between their targets. Competing endogenous RNAs
(ceRNAs) can in turn regulate each other through miRNA-mediated crosstalk.
Albeit potentially weak, ceRNA interactions can occur both dynamically,
affecting e.g. the regulatory clock, and at stationarity, in which case ceRNA
networks as a whole can be implicated in the composition of the cell's
proteome. Many features of ceRNA interactions, including the conditions under
which they become significant, can be unraveled by mathematical and in silico
models. We review the understanding of the ceRNA effect obtained within such
frameworks, focusing on the methods employed to quantify it, its role in the
processing of gene expression noise, and how network topology can determine its
reach.Comment: review article, 29 pages, 7 figure
Predictors of reading literacy for first and second language learners
- Author
- A Brooks
- A Gottardo
- A Wigfield
- Andrea Netten
- C Aarnoutse
- CA Perfetti
- CA Perfetti
- CE Snow
- CP Proctor
- D Dickinson
- E Geva
- F Genesee
- G Driessen
- G Staphorsius
- GN Marks
- I Lundberg
- Instituut voor Toegepaste Sociologie (ITS).
- International Association for the Evaluation of Educational Achievement (IEA)
- ITS
- IVS Mullis
- IVS Mullis
- J Cummins
- J Janssen
- JL Meece
- JT Guthrie
- K Aunola
- K Jöreskog
- K Koda
- K Stanovich
- KE Cox
- L Hu
- L Verhoeven
- L Verhoeven
- Ludo Verhoeven
- M Diepen van
- M Droop
- M Wang
- Mienke Droop
- MK Lerkkanen
- NK Lesaux
- Organisation for Economic Co-operation Development (OECD)
- P Tabors
- PB Gough
- PF Jong de
- R Serpell
- RD Tiu
- RM Joshi
- RM Joshi
- SM Adlof
- W Elsäcker van
- WA Hoover
- Publication venue
- Springer Netherlands
- Publication date
- 01/01/2010
- Field of study
In this study an attempt was made to construct a multi-factor model predicting the development of reading literacy in the upper grades of primary school in the Netherlands for subgroups of 729 first language (L1) learners and 93 second language (L2) learners. Following a longitudinal design, it was explored to what extent the variation in reading literacy development in L1 and L2 from grade 4 to grade 6 can be explained from children’s word decoding, language, mathematics and nonverbal reasoning skills, reading motivation and self confidence as well as their home reading resources. The results showed that L1 and L2 learners differed in reading literacy skills, language, mathematics, and reasoning skills. Structural equation modelling showed that the reading literacy development in both L1 and L2 learners could be explained from decoding, language, mathematics and reasoning skills, as well as their motivation and self-confidence. A striking difference was the fact that home reading resources had an impact on reading literacy in L1 learners but not in L2 learners
Worldwide impacts of climate change on energy for heating and cooling
- Author
- A Bernard
- Amit Kanudia
- B Hamududu
- B Lehner
- B Thomas
- D Rübbelke
- D Vuuren van
- E Akpinar-Ferrand
- F Babonneau
- F Eboli
- Frédéric Babonneau
- G Schoenau
- H Haberl
- I Ward
- J Dimitropoulos
- J Harrison
- K Fraedrich
- K Linnerud
- M Dolinar
- M Isaac
- M Labriet
- M Williamson
- Marc Vielle
- Maryse Labriet
- Neil R. Edwards
- PB Holden
- Philip B. Holden
- R Loulou
- R Loulou
- R Schaeffer
- R Warren
- Richard Loulou
- S Paltsev
- Santosh R. Joshi
- T Mideksa
- TJ Wilbanks
- X Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 26/09/2013
- Field of study
The energy sector is not only a major contributor to greenhouse gases, it is also vulnerable to climate change and will have to adapt to future climate conditions. The objective of this study is to analyze the impacts of changes in future temperatures on the heating and cooling services of buildings and the resulting energy and macro-economic effects at global and regional levels. For this purpose, the techno-economic TIAM-WORLD (TIMES Integrated Assessment Model) and the general equilibrium GEMINI-E3 (General Equilibrium Model of International-National Interactions between Economy, Energy and Environment) models are coupled with a climate model, PLASIM-ENTS (Planet-Simulator - Efficient Numerical Terrestrial Scheme). The key results are as follows. At the global level, the climate feedback induced by adaptation of the energy system to heating and cooling is found to be insignificant, partly because heating and cooling-induced changes compensate and partly because they represent a limited share of total final energy consumption. However, significant changes are observed at regional levels, more particularly in terms of addi- tional power capacity required to satisfy additional cooling services, resulting in increases in electricity prices. In terms of macro-economic impacts, welfare gains and losses are associated more with changes in energy exports and imports than with changes in energy consumption for heating and cooling. The rebound effect appears to be non-negligible. To conclude, the coupling of models of different nature was successful and showed that the energy and economic impacts of climate change on heating and cooling remain small at the global level, but changes in energy needs will be visible at more local scale
The Set2/Rpd3S Pathway Suppresses Cryptic Transcription without Regard to Gene Length or Transcription Frequency
- Author
- AA Joshi
- Andrew B. Nobel
- Andrey A. Shabalin
- B Li
- B Li
- B Li
- B Li
- B Rao
- BD Strahl
- Bhargavi Rao
- Brian D. Strahl
- C-K Lee
- CD Kaplan
- Colin R. Lickwar
- DK Pokholok
- DWK Andrews
- E Segal
- FCP Holstege
- G-C Yuan
- GJ Hogan
- H Cedar
- I Whitehouse
- IP Ioshikhes
- J Bai
- JA Knezetic
- Jason D. Lieb
- JD Anderson
- JD Lieb
- KO Kizer
- Laura Rusche
- M Huarte
- M-C Keogh
- MJ Carrozza
- ML Youdell
- NJ Krogan
- PB Mason
- T Xiao
- V Cheung
- X Liu
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
In cells lacking the histone methyltransferase Set2, initiation of RNA polymerase II transcription occurs inappropriately within the protein-coding regions of genes, rather than being restricted to the proximal promoter. It was previously reported that this “cryptic” transcription occurs preferentially in long genes, and in genes that are infrequently transcribed. Here, we mapped the transcripts produced in an S. cerevisiae strain lacking Set2, and applied rigorous statistical methods to identify sites of cryptic transcription at high resolution. We find that suppression of cryptic transcription occurs independent of gene length or transcriptional frequency. Our conclusions differ with those reported previously because we obtained a higher-resolution dataset, we accounted for the fact that gene length and transcriptional frequency are not independent variables, and we accounted for several ascertainment biases that make cryptic transcription easier to detect in long, infrequently transcribed genes. These new results and conclusions have implications for many commonly used genomic analysis approaches, and for the evolution of high-fidelity RNA polymerase II transcriptional initiation in eukaryotes
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV 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
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aperio Bella L
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce AT
- Arfaoui S
- Arguin JF
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- ATLAS Collaboration The
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Backus Mayes J
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro Guimarães da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartsch V
- Basye A
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Bauer F
- Bawa HS
- Beale S
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker K
- Becker S
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behar Harpaz S
- Belanger-Champagne C
- Bell PJ
- Bell WH
- Bella G
- Bellagamba L
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bendtz K
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez Garcia JA
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernat P
- Bernhard R
- Bernius C
- Bernlochner FU
- Berry T
- Bertella C
- Bertin A
- Bertolucci F
- Besana MI
- Besjes GJ
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bittner B
- Black CW
- Black JE
- Black KM
- Blair RE
- Blanchard JB
- Blazek T
- Bloch I
- Blocker C
- Blocki J
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boek TT
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- Bogaerts JA
- Bogdanchikov A
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- Bohm J
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bomben M
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- Boonekamp M
- Bordoni S
- Borer C
- Borisov A
- Borissov G
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- Bortfeldt J
- Bortolotto V
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- Boscherini D
- Bosman M
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- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
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- Bozovic-Jelisavcic I
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- Brau JE
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- Brazzale SF
- Brelier B
- Bremer J
- Brendlinger K
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- Bristow TM
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- Bruckman de Renstrom PA
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- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Byszewski M
- Büscher V
- Cabrera Urbán S
- Caforio D
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camacho Toro R
- Camarri P
- Cameron D
- Caminada LM
- Caminal Armadans R
- Campana S
- Campanelli M
- Canale V
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- Cantero J
- Cantrill R
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- Capeans Garrido MD
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- Carrillo-Montoya GD
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- Castro NF
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- Chavez Barajas CA
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- Chekanov S
- Chekulaev SV
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- Chelstowska MA
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- Chernyatin V
- Cheu E
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- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Choudalakis G
- Chouridou S
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- Christidi IA
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- Chromek-Burckhart D
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- Chudoba J
- Ciapetti G
- Ciftci AK
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- Cinca D
- Cindro V
- Ciocio A
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- Citron ZH
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- Conventi F
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- Cranmer K
- Crescioli F
- Cristinziani M
- Crosetti G
- Crépé-Renaudin S
- Cuciuc CM
- Cuenca Almenar C
- Cuhadar Donszelmann T
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- Curatolo M
- Curtis CJ
- Cuthbert C
- Cwetanski P
- Czirr H
- Czodrowski P
- Czyczula Z
- Côté D
- D'Auria S
- D'Onofrio M
- D'Orazio A
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dafinca A
- Dai T
- Dallaire F
- Dallapiccola C
- Dam M
- Damiani DS
- Danielsson HO
- Dao V
- Darbo G
- Darlea GL
- Dassoulas JA
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davignon O
- Davison AR
- Davygora Y
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Asmundis R
- De Castro S
- De Cecco S
- de Graat J
- De Groot N
- de Jong P
- De La Taille C
- De la Torre H
- De Lorenzi F
- De Nooij L
- De Pedis D
- De Salvo A
- De Sanctis U
- De Santo A
- De Vivie De Regie JB
- De Zorzi G
- De K
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dechenaux B
- Dedovich DV
- Degenhardt J
- Del Peso J
- Del Prete T
- Delemontex T
- Deliyergiyev M
- Dell'acqua A
- Dell'asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demirkoz B
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deviveiros PO
- Dewhurst A
- Dewilde B
- Dhaliwal S
- Dhullipudi R
- Di Ciaccio A
- Di Ciaccio L
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Luise S
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Diaz MA
- Diehl EB
- Dietrich J
- Dietzsch TA
- Diglio S
- Dindar Yagci K
- Dingfelder J
- Dinut F
- Dionisi C
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- do Vale MA
- Do Valle Wemans A
- Doan TK
- Dobbs M
- Dobos D
- Dobson E
- Dodd J
- Doglioni C
- Doherty T
- Dohmae T
- Doi Y
- Dolejsi J
- Dolezal Z
- Dolgoshein BA
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- Yamaguchi H
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- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki T
- Yamazaki Y
- Yan Z
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- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yasu Y
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- Yen AL
- Yilmaz M
- Yoosoofmiya R
- 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
- Zeniš 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
- Zhou B
- Zhou N
- Zhou Y
- 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
- Zivković 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 (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) 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<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Measurement of the production of a W boson in association with a charm quark in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
- A Hasib
- A Martin
- A. A. Carter
- A. A. E. Bannoura
- A. A. Grillo
- A. A. Komar
- A. A. Korol
- A. A. Minaenko
- A. A. Nepomuceno
- A. A. Snesarev
- A. A. Solodkov
- A. A. Talyshev
- A. Ahmad
- A. Aloisio
- A. Alonso
- A. Altheimer
- A. Amorim
- A. Andreazza
- A. Angerami
- A. Annovi
- A. Antonaki
- A. Antonov
- A. Artamonov
- A. Ashkenazi
- A. B. Fenyuk
- A. Bangert
- A. Baroncelli
- A. Bassalat
- A. Basye
- A. Beddall
- A. Bellerive
- A. Belloni
- A. Bingul
- A. Bocci
- A. Bogouch
- A. Borisov
- A. Boveia
- A. Brandt
- A. Bruni
- A. Buzatu
- A. C. Bundock
- A. C. Daniells
- A. C. Florez Bustos
- A. C. König
- A. C. Martyniuk
- A. C. Schaffer
- A. Campoverde
- A. Canepa
- A. Castelli
- A. Catinaccio
- A. Cattai
- A. Cerri
- A. Cervelli
- A. Chafaq
- A. Chegwidden
- A. Cheplakov
- A. Chilingarov
- A. Chitan
- A. Ciocio
- A. Clark
- A. Coccaro
- A. Corso-Radu
- A. Cortes-Gonzalez
- A. D. Hawkins
- A. D. Pilkington
- A. Dafinca
- A. De Salvo
- A. De Santo
- A. Dell’Acqua
- A. Demilly
- A. Dewhurst
- A. Di Ciaccio
- A. Di Domenico
- A. Di Girolamo
- A. Di Mattia
- A. Di Simone
- A. Dimitrievska
- A. Do Valle Wemans
- A. Doria
- A. Dos Anjos
- A. Dudarev
- A. Durglishvili
- A. E. Barton
- A. E. Kiryunin
- A. E. Loevschall-Jensen
- A. Ereditato
- A. F. Saavedra
- A. Farbin
- A. Farilla
- A. Favareto
- A. Ferrari
- A. Ferrer
- A. Ferretto Parodi
- A. Filipčič
- A. Firan
- A. Floderus
- A. Formica
- A. Forti
- A. G. Bogdanchikov
- A. G. Buckley
- A. G. Goussiou
- A. G. Leister
- A. G. Myagkov
- A. G. Olchevski
- A. Gabrielli
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- X. Ruan
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- X. Sun
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- X. Zhang
- X. Zhuang
- Y. A. Kurochkin
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- Y. Arai
- Y. Azuma
- Y. B. Pan
- Y. Bai
- Y. Benhammou
- Y. Chen
- Y. Cheng
- Y. Coadou
- Y. Davygora
- Y. Enari
- Y. F. Ryabov
- Y. Fang
- Y. Hasegawa
- Y. Hernández Jiménez
- Y. Huang
- Y. Ikegami
- Y. Inamaru
- Y. J. Schnellbach
- Y. Jiang
- Y. Kataoka
- Y. Komori
- Y. Kulchitsky
- Y. Li
- Y. Liu
- Y. Makida
- Y. Ming
- Y. Munwes
- Y. Nagai
- Y. Nagasaka
- Y. Nakahama
- Y. Ninomiya
- Y. Okumura
- Y. Oren
- Y. Pylypchenko
- Y. Rozen
- Y. S. Gao
- Y. Sakurai
- Y. Sasaki
- Y. Silver
- Y. Smirnov
- Y. Sugaya
- Y. Suzuki
- Y. Takahashi
- Y. Takubo
- Y. Tayalati
- Y. Unno
- Y. V. Grishkevich
- Y. Wu
- Y. Yamaguchi
- Y. Yamazaki
- Y. Yang
- Y. Yasu
- Y. Zhu
- Yu. A. Tikhonov
- Z. Barnovska
- Z. Czyczula
- Z. D. Greenwood
- Z. Dolezal
- Z. Gecse
- Z. H. Citron
- Z. Hajduk
- Z. Hubacek
- Z. J. Grout
- Z. Kohout
- Z. L. Ren
- Z. Liang
- Z. Marshall
- Z. Rurikova
- Z. V. Krumshteyn
- Z. Vykydal
- Z. Weng
- Z. Yan
- Z. Zhang
- Z. Zhao
- Z. Zinonos
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The production of a W boson in association with a single charm quark is studied using 4.6 fb−1 of pp collision data at s√ = 7 TeV collected with the ATLAS detector at the Large Hadron Collider. In events in which a W boson decays to an electron or muon, the charm quark is tagged either by its semileptonic decay to a muon or by the presence of a charmed meson. The integrated and differential cross sections as a function of the pseudorapidity of the lepton from the W-boson decay are measured. Results are compared to the predictions of next-to-leading-order QCD calculations obtained from various parton distribution function parameterisations. The ratio of the strange-to-down sea-quark distributions is determined to be 0.96+0.26−0.30 at Q 2 = 1.9 GeV2, which supports the hypothesis of an SU(3)-symmetric composition of the light-quark sea. Additionally, the cross-section ratio σ(W + +c¯¯)/σ(W − + c) is compared to the predictions obtained using parton distribution function parameterisations with different assumptions about the s−s¯¯¯ quark asymmetry
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
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- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
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- Amram N
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- Anders G
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- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
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- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
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- Armbruster AJ
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- Bangert A
- Bansal V
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- Caminal Armadans R
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- Castillo IS
- Castillo LRF
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- Chernyatin V
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- De Pedis D
- De Regie JBDV
- de Renstrom PAB
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- Delsart PA
- Deluca C
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- Demilly A
- Demirkoz B
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- Derue F
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- Deviveiros PO
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
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- Di Simone A
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- Dueren M
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- Dwuznik M
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- Ekelof T
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- El Moursli A
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- Enari Y
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- Engelmann R
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- Erdmann J
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- Ereditato A
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- Eriksson D
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- Errede D
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- Errede S
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- Ertel E
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- Escalier M
- Escalier M
- Esch H
- Esch H
- Escobar C
- Escobar C
- Espinal Curull X
- Espinal Curull X
- Esposito B
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- Etienne F
- Etienne F
- Etienvre AI
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- Etzion E
- Etzion E
- Evans H
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- Fabbri L
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- Facini G
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- Fakhrutdinov RM
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- Faltova J
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- Fang Y
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- Farooque T
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- Farrell S
- Farrell S
- Farrington SM
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- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
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- Fassouliotis D
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- Favareto A
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- Fayard L
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- Federic P
- Federic P
- Fedin OL
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- Fedorko W
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- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
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- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
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- Fenyuk AB
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- Fernando W
- Fernando W
- Ferrag S
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- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
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- Ferrari A
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- Ferrari P
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- Ferretti C
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- Fiascaris M
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- Fiedler F
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- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
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- Fincke-Keeler M
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- Fiolhais MCN
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- Fiorini L
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- Firan A
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- Fischer J
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- Fisher MJ
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- Fitzgerald EA
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- Fleck I
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- Fleischmann P
- Fleischmann P
- Fleischmann S
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- Fletcher G
- Fletcher G
- Fletcher GT
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- Floderus A
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- Florez Bustos AC
- Flowerdew MJ
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- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
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- Fournier D
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- Francavilla P
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- Franklin M
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- Franz S
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- French ST
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- Friedrich F
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- Fulsom BG
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- Gabizon O
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- Gabrielli A
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- Gadatsch S
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- Gadomski S
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- Gagliardi G
- Gagliardi G
- Gagnon P
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- Galea C
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- Galhardo B
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- Gallas EJ
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- Gallo V
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- Gallop BJ
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- Gallus P
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- Gandrajula RP
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- Gao J
- Gao YS
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- Gaob J
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- Garcia BRM
- Garcia C
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- Garcia JAB
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- Gardner RW
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- Garelli N
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- Garonne V
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- Garrido MDMC
- Gatti C
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- Gaudio G
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- Gaur B
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- Gauzzi P
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- Gavrilenko IL
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- Gay C
- Gay C
- Gaycken G
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- Gazis EN
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- Ge P
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- Gecse Z
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- Gee CNP
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- Geerts DAA
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- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
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- Gemme C
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- Gemmell A
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- Genest MH
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- Gentile S
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- George M
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- George S
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- Gerbaudo D
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- Gershon A
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- Ghazlane H
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- Ghodbane N
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- Giacobbe B
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- Giagu S
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- Giangiobbe V
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- Giannetti P
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- Gillberg D
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- Gillman AR
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- Gingrich DM
- Gingrich M
- Giokaris N
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- Giordani MP
- Giordani MP
- Giordano R
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- Giorgi FM
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- Giraud PF
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- Giugni D
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- Giuliani C
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- Giunta M
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- Gjelsten BK
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- Gorbounov PA
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- Gordon HA
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- Gorelov I
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- Gorini B
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- Gorini E
- Gorini E
- Gorisek A
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- Gornicki E
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- Goshaw AT
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- Gostkin MI
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for 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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- 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 τ 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, φ, 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 β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
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- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
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- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
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- Andreazza A
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- Angelidakis S
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- Anh TV
- Anisenkov AV
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- Antonaki A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
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