969 research outputs found
Molecular diversity of anthracnose pathogen populations associated with UK strawberry production suggests multiple introductions of three different Colletotrichum species.
- Author
- AG Buddie
- Antonio Zapparata
- AR Ureña-Padilla
- B Denoyes-Rothan
- B Denoyes-Rothan
- BC Sutton
- BJ Smith
- BS Weir
- C Garrido
- Charles R. Lane
- CM Howard
- CM Howard
- D Jones
- DW Simpson
- EJ Calleja
- Eric Holub
- F Ronquist
- Giovanni Vannacci
- JC Guerber
- JL Maas
- K Tamura
- M Kearse
- MA Whitelaw-Weckert
- Mark Gijzen
- MG Beech
- Michael R. Thon
- MZ Du
- NA Peres
- P Talhinhas
- PV Martínez-Culebras
- R Baroncelli
- R Baroncelli
- R Baroncelli
- R Baroncelli
- R Sepp
- Riccardo Baroncelli
- RJ Mason-Gamer
- RJ O'Connell
- S Freeman
- S Freeman
- S Sreenivasaprasad
- S Sreenivasaprasad
- Sabrina Sarrocco
- Serenella A. Sukno
- Surapareddy Sreenivasaprasad
- U Damm
- W Van Hemelrijck
- ZJ Jelev
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2015
- Field of study
Fragaria × ananassa (common name: strawberry) is a globally cultivated hybrid species belonging to Rosaceae family. Colletotrichum acutatum sensu lato (s.l.) is considered to be the second most economically important pathogen worldwide affecting strawberries. A collection of 148 Colletotrichum spp. isolates including 67 C. acutatum s.l. isolates associated with the phytosanitary history of UK strawberry production were used to characterize multi-locus genetic variation of this pathogen in the UK, relative to additional reference isolates that represent a worldwide sampling of the diversity of the fungus. The evidence indicates that three different species C. nymphaeae, C. godetiae and C. fioriniae are associated with strawberry production in the UK, which correspond to previously designated genetic groups A2, A4 and A3, respectively. Among these species, 12 distinct haplotypes were identified suggesting multiple introductions into the country. A subset of isolates was also used to compare aggressiveness in causing disease on strawberry plants and fruits. Isolates belonging to C. nymphaeae, C. godetiae and C. fioriniae representative of the UK anthracnose pathogen populations showed variation in their aggressiveness. Among the three species, C. nymphaeae and C. fioriniae appeared to be more aggressive compared to C. godetiae. This study highlights the genetic and pathogenic heterogeneity of the C. acutatum s.l. populations introduced into the UK linked to strawberry production
Influenza A H5N1 and HIV co-infection: case report
- Author
- A Gambotto
- Annette Fox
- BS Bender
- Cameron Simmons
- DM Thea
- H Valdez
- H Yu
- Heiman Wertheim
- IN Kandun
- JD Barbour
- JD Miller
- Jeremy Farrar
- JS Peiris
- K Kedzierska
- KM Kunisaki
- Le Nguyen Minh Hoa
- MD de Jong
- N Hasejima
- Nguyen Hong Ha
- Nguyen Tien Lam
- Nguyen Van Kinh
- NT Liem
- Peter Horby
- R Perez-Padilla
- S Garcia Garcia
- T Chotpitayasunondh
- T Ohnishi
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>The role of adaptive immunity in severe influenza is poorly understood. The occurrence of influenza A/H5N1 in a patient with HIV provided a rare opportunity to investigate this.</p> <p>Case Presentation</p> <p>A 30-year-old male was admitted on day 4 of influenza-like-illness with tachycardia, tachypnea, hypoxemia and bilateral pulmonary infiltrates. Influenza A/H5N1 and HIV tests were positive and the patient was treated with Oseltamivir and broad-spectrum antibiotics. Initially his condition improved coinciding with virus clearance by day 6. He clinically deteriorated as of day 10 with fever recrudescence and increasing neutrophil counts and died on day 16. His admission CD4 count was 100/μl and decreased until virus was cleared. CD8 T cells shifted to a CD27<sup>+</sup>CD28<sup>- </sup>phenotype. Plasma chemokine and cytokine levels were similar to those found previously in fatal H5N1.</p> <p>Conclusions</p> <p>The course of H5N1 infection was not notably different from other cases. Virus was cleared despite profound CD4 T cell depletion and aberrant CD8 T cell activation but this may have increased susceptibility to a fatal secondary infection.</p
Two-pion Bose-Einstein correlations in central Pb-Pb collisions at sNN = 2.76 TeV
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- Rui R.
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- T.S. R\ue4ih\ue4af
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- U. Fuchsf
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- V. Posp\ued\u161il ay
- V. Puninbk
- V. Samsonov au
- V. Vechernin t
- V. Wagneray
- V.R. Loggins at
- Venaruzzo M.
- W. Carena f
- W. Jung k
- W. Perytcn
- W. Rieglerf
- W.H. Trzaskaaf
- W.J. Parks
- X. Cai bn
- X. Li cz
- X. Lopezak
- X. Yuanbn
- X. Zhang bn
- X. Zhubn
- X.-G. Lu bl
- Y. Berdnikov au
- Y. Corrales Morales ah
- Y. Delgado Mercado bo
- Y. Hori cr
- Y. Kharlovbd
- Y. Kucheriaevm
- Y. Kwoncw
- Y. Le Bornec bg
- Y. Maobn
- Y. Martynov p
- Y. Miake bu
- Y. Pachmayerbl
- Y. Pestovdf
- Y. Schutzaa
- Y. Sibiriakm
- Y. Vinogradov bk
- Y. Wangbl
- Y. Wangbn
- Y. Zoccarato bq
- Y.P. Viyogi i
- Y.W. Baekk
- Z. Ahammed i
- Z. Buthelezi bm
- Z. Conesa del Valle aa
- Z. Vilakazi bm
- Z. Yinbn
- Z.L. Matthews an
- Publication venue
- 'Elsevier BV'
- Publication date
- 21/12/2010
- Field of study
The first measurement of two-pion Bose-Einstein correlations in central Pb-Pb
collisions at sNN=2.76 TeV at the Large Hadron Collider is
presented. We observe a growing trend with energy now not only for the
longitudinal and the outward but also for the sideward pion source radius. The
pion homogeneity volume and the decoupling time are significantly larger than
those measured at RHIC.Comment: 17 pages, 5 captioned figures, 1 table, authors from page 12,
published version, figures at
http://aliceinfo.cern.ch/ArtSubmission/node/388
Effective Rheology of Bubbles Moving in a Capillary Tube
- Author
- Abelev B
- Adam J
- Adamova D
- Adare AM
- Aggarwal MM
- Agocs AG
- Agostinelli A
- Ahammed Z
- Ahmad N
- Ahn SU
- Akindinov A
- Alaniz EC
- Aleksandrov D
- Alessandro B
- Alici A
- Alkin A
- Alme J
- Alt T
- Altini V
- Altinpinar S
- Altsybeev I
- Andrei C
- Andronic A
- Anguelov V
- Anielski J
- Anson C
- Anticic T
- Antinori F
- Antonioli P
- Aphecetche L
- Appelshauser H
- Arbor N
- Arcelli S
- Arend A
- Armesto N
- Arnaldi R
- Aronsson T
- Arsene IC
- Arslandok M
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
- Bach M
- Badala A
- Baek YW
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Baldit A
- Ban J
- Baral RC
- Barbera R
- Bari DD
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barros GOVD
- Barroso VC
- Bartke J
- Basile M
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann C
- Bearden IG
- Beck H
- Belikov I
- Bellini F
- Bellwied R
- Belmont-Moreno E
- Bencedi G
- Beole S
- Berceanu I
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bergmann C
- Berzano D
- Betev L
- Bhasin A
- Bhati AK
- Bianchi L
- Bianchi N
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- Bjelogrlic S
- Blanco F
- Blanco F
- Blau D
- Blume C
- Boccioli M
- Bock N
- Bogdanov A
- Boggild H
- Bogolyubsky M
- Boldizsar L
- Bombara M
- Book J
- Borel H
- Borissov A
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- Bose S
- Bossu F
- Botje M
- Bottger S
- Boyer B
- Braidot E
- Braun-Munzinger P
- Bregant M
- Breitner T
- Browning TA
- Broz M
- Brun R
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Bufalino S
- Bugaiev K
- Busch O
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- Buthelezi Z
- Caffarri D
- Cahuantzi MR
- Cai X
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- Carena F
- Carena W
- Carminati F
- Caro AD
- Castellanos JC
- Castro XS
- Casula EAR
- Cataldo GD
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- Chapeland S
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- Chinellato DD
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- Chojnacki M
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- Contreras JG
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- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
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- Cuveland JD
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- Dalsgaard HH
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- Delagrange H
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- Dominguez I
- Don CKK
- Donigus B
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- Dupieux P
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- Guilbaud M
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- Gutbrod H
- Gutierrez CG
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- Kaidalov AB
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- Knichel ML
- Knospe AG
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- Kohler MK
- Kolk NVD
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- Konevskikh A
- Korneev A
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- Kowalski M
- Kox S
- Kral J
- Kralik I
- Kramer F
- Kraus I
- Krawutschke T
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- Krivda M
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- Kucheriaev Y
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- Kuijer PG
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- Kuryakin A
- Kushpil S
- Kushpil V
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- Kweon MJ
- Kwon Y
- Lakomov I
- Langoy R
- Lara C
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- Lee SC
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- Lehnert J
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- Lezama EP
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- Lindal S
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- Loenne PI
- Loggins VR
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- Lohner D
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- Lovhoiden G
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- Luo J
- Luparello G
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- Maevskaya A
- Mager M
- Mahapatra DP
- Maire A
- Majumdar AKD
- Majumdar MRD
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- Malaev M
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- Malzacher P
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- Marchisone M
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- Martinengo P
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- Masera M
- Masoni A
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- Mastroserio A
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- Mauro AD
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- Mazzoni MA
- Meddi F
- Meethaleveedu GK
- Menchaca-Rocha A
- Meres M
- Miake Y
- Milano L
- Milosevic J
- Mischke A
- Mishra AN
- Miskowiec D
- Mitu C
- Mlynarz J
- Mohanty AK
- Mohanty B
- Molina RA
- Molnar L
- Monteno M
- Montero AJR
- Montes E
- Montoya CAC
- Monzon IL
- Moon T
- Morales YC
- Morando M
- Moretto S
- Morsch A
- Muccifora V
- Mudnic E
- Muhuri S
- Muller H
- Munhoz MG
- Munoz GT
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- Nappi E
- Nattrass C
- Naumov NP
- Navin S
- Nayak TK
- Nazarenko S
- Nazarov G
- Nedosekin A
- Nezza PD
- Nicassio M
- Nielsen BS
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- Palmeri A
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- Pappalardo GS
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- Passfeld A
- Pastircak B
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- Truesdale D
- Trzaska WH
- Tsuji T
- Tumkin A
- Turrisi R
- Tveter TS
- Ulery J
- Ullaland K
- Ulrich J
- Uras A
- Urban J
- Urciuoli GM
- Usai GL
- Uysal AK
- Vajzer M
- Vala M
- Valle ZCD
- Vallero S
- Vannucci L
- Vargas A
- Vargas HL
- Varma R
- Vasileiou M
- Vasiliev A
- Vasquez MAS
- Vechernin V
- Velasquez AO
- Veldhoen M
- Venaruzzo M
- Vercellin E
- Vergara S
- Vernekohl DC
- Vernet R
- Verweij M
- Vickovic L
- Viesti G
- Vikhlyantsev O
- Vilakazi Z
- Villar EC
- Vinogradov A
- Vinogradov L
- Vinogradov Y
- Virgili T
- Viyogi YP
- Vodopyanov A
- Voloshin K
- Voloshin S
- Volpe G
- Vranic D
- Vrlakova J
- Vulpescu B
- Vyushin A
- Vyvre PV
- Wagner B
- Wagner V
- Wan R
- Wang D
- Wang M
- Wang Y
- Wang Y
- Watanabe K
- Wessels JP
- Westerhoff U
- Wiechula J
- Wikne J
- Wilde M
- Wilk A
- Wilk G
- Williams MCS
- Windelband B
- Yang H
- Yang S
- Yasnopolskiy S
- Yi J
- Yin Z
- Yokoyama H
- Yoo IK
- Yoon J
- Yu W
- Yuan X
- Yushmanov I
- Zach C
- Zampolli C
- Zaporozhets S
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zelnicek P
- Zetina LM
- Zgura IS
- Zhalov M
- Zhang X
- Zhou D
- Zhou F
- Zhou Y
- Zhu X
- Zichichi A
- Zimmermann A
- Zinovjev G
- Zoccarato Y
- Zynovyev M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 16/03/2012
- Field of study
We calculate the average volumetric flux versus pressure drop of bubbles
moving in a single capillary tube with varying diameter, finding a square-root
relation from mapping the flow equations onto that of a driven overdamped
pendulum. The calculation is based on a derivation of the equation of motion of
a bubble train from considering the capillary forces and the entropy production
associated with the viscous flow. We also calculate the configurational
probability of the positions of the bubbles.Comment: 4 pages, 1 figur
Suppression of charged particle production at large transverse momentum in central Pb-Pb collisions at sNN=2.76 TeV
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- C. Cavicchioli f
- C. Cheshkovbp
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- C. Hadjidakisbf
- C. Hern\ue1ndez s
- C. Ivans
- C. Klein-B\uf6sing ap
- C. Kottachchi Kankanamge Don at
- C. Kuhn as
- C. Larav
- C. Lazzeroni an
- C. Lippmann f
- C. Loizidesct
- C. Luzzi f
- C. Mitu ca
- C. Nattrass db
- C. Nygaard ar
- C. Oppedisano n
- C. Pajaresad
- C. Pettaam
- C. Royaa
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- C. Schiauau
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- C. Soos f
- C. Suire bf
- C. Tagridis cm
- C. Terrevoli r
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- C.H. Christensen ar
- C.W. Fabjanf
- D. Adamov\ue1c
- D. Aleksandrovm
- D. Blaum
- D. Budnikovbj
- D. Caffarri y
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- D. De Gruttolacd
- D. Di Bari r
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- D. Perini f
- D. Perrino r
- D. R\uf6hrich a
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- D. Sakata bt
- D. Silvermyr ae
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- E. Almar\ue1z Avi\uf1a h
- E. Belmont-Moreno h
- E. Berdermanns
- E. Biolcati ah
- E. Bruna d
- E. Calvo Villar bn
- E. Chiavassa n
- E. Cresciobv
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- E. D\ue9nes g
- E. Fragiacomo cl
- E. Gladysz-Dziadus ao
- E. Incani cf
- E. Kang k
- E. Karpechevck
- E. Korna\ub4s ao
- E. Kryshenau
- E. L\uf3pez Torres b
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- E. Quercigh f
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- E. Zabrodin bg
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- F. Antinori y
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- G. Simonetti f
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- G. Stefanini f
- G. Steynbl
- G. Tejeda Mu\uf1oz bw
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- H. Beck ab
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- I. Altsybeevt
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- I. Berceanuu
- I. Cort\ue9s Maldonado bw
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- I. Dom\uednguez by
- I. H\u2c7rivn\ue1\u2c7cov\ue1 bf
- I. Ilkivcg
- I. Kisel v
- I. Kr\ue1likal
- I. Krauscv
- I. Le\uf3n Monz\uf3nco
- I. Maldonado Cervantes by
- I. Martashvili db
- I. Otterlundbs
- I. Pshenichnov ck
- I. Rusanovf
- I. Stanca
- I. Szarkabi
- I. Yushmanovm
- I. Zguraca
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- J. B\ue1nal
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- L. Monta\uf1o Zetinabv
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- L. Pinsky ba
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- M. Lenhardt aa
- M. Lunardony
- M. Magerf
- M. Malaev au
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- M. Mastromarco ce
- M. Montenon
- M. Morando y
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- M. Rammler ap
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- M. Shimomura bt
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- M. Tavletf
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- M. van Leeuwen br
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- M. Venaruzzo bh
- M. Verweij br
- M. Wildeap
- M. Zhalovau
- M. Zynovyev p
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- M.A. Mazzoni ch
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- M.D. Azmi j
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- M.I. Mart\uednez bw
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- M.R. Dutta Majumdar i
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- N. Armestoad
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- P. Braun-Munzinger s
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- P. Christakoglou br
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- P. Ghosh i
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- P. Riedlerf
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- W.H. Trzaskaaf
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- X. Zhang bm
- X.-G. Lubk
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- Y. Hori cr
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- Y. Kucheriaevm
- Y. Kwoncw
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- Y. Maobm
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- Publication venue
- 'Elsevier BV'
- Publication date
- 07/12/2010
- Field of study
Inclusive transverse momentum spectra of primary charged particles in Pb-Pb
collisions at sNN = 2.76 TeV have been measured by the ALICE
Collaboration at the LHC. The data are presented for central and peripheral
collisions, corresponding to 0-5% and 70-80% of the hadronic Pb-Pb cross
section. The measured charged particle spectra in ∣η∣<0.8 and 0.3<pT<20 GeV/c are compared to the expectation in pp collisions at the same
sNN, scaled by the number of underlying nucleon-nucleon
collisions. The comparison is expressed in terms of the nuclear modification
factor RAA. The result indicates only weak medium effects (RAA≈ 0.7) in peripheral collisions. In central collisions, RAA
reaches a minimum of about 0.14 at pT=6-7GeV/c and increases
significantly at larger pT. The measured suppression of high-pT particles is stronger than that observed at lower collision energies,
indicating that a very dense medium is formed in central Pb-Pb collisions at
the LHC.Comment: 15 pages, 5 captioned figures, 3 tables, authors from page 10,
published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/98
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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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
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- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
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- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
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- Amidei D
- Amor Dos Santos SP
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- Castillo Gimenez V
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- Castro NF
- Catinaccio A
- Catmore JR
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- Cochran J
- Cohen H
- Coimbra AEC
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- Constantinescu S
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- Cranmer K
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- Creager RA
- Crepe-Renaudin S
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- Cueto A
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- da Costa JBG
- Da Fonseca Pinto J
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- Dabrowski W
- Dachs F
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- Dallapiccola C
- Dam M
- Damazio DO
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- Dandoy JR
- Daneri MF
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- De Asmundis R
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- De Groot N
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- De Lima RT
- De Maria A
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- De Regie JBDV
- de Renstrom PAB
- De Sa RCL
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- Debenedetti C
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- Demichev M
- Demontigny G
- Denisov SP
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- Dette K
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- 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
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Zmouchko VV
- Zobernig G
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- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Observation of associated near-side and away-side long-range correlations in √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
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- Zevi Della Porta G
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- 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 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
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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 direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
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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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