1,502 research outputs found
Surviving pediatric intensive care: physical outcome after 3 months
- Author
- A Balluffi
- A Diaz-Caneja
- A Taylor
- AF Klassen
- AL Morrison
- Albert P. Bos
- CM Buysse
- DC Angus
- DH Fiser
- DH Fiser
- DH Fiser
- DM Needham
- DW Dowdy
- DW Dowdy
- EH Rijen van
- H Knoester
- Hendrika Knoester
- J Lopez-Herce
- JC Wain
- JM Fellick
- JM Tilford
- K Samuelson
- KD Dominguez
- LR Sorce
- M Jayshree
- M Maat
- Madelon B. Bronner
- MC McCormick
- NA Halpern
- RC Savage
- RJ Gemke
- S Jones
- S Kuhle
- T Horisberger
- TA Williams
- TM Davey
- TR Ehrlich
- W Butt
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2008
- Field of study
Objective: This study investigated the prevalence and nature of physical and neurocognitive sequelae in pediatric intensive care unit ( PICU) survivors. Design and setting: Prospective follow-up study 3 months after discharge from a 14-bed tertiary PICU in The Netherlands. Patients and participants: The families of 250 previously healthy children unexpectedly admitted to the PICU were invited to visit the outpatient follow-up clinic for structured medical examination of the child 3 months after discharge; 186 patients were evaluated. Measurements and results: Pediatric Cerebral Performance Category ( PCPC) and Pediatric Overall Performance Category ( POPC) values were determined at PICU discharge, at the outpatient follow-up clinic, and retrospectively before admission to the PICU. We found that 69% of children had physical sequelae. In 30% of cases these were caused by a previously unknown illness and in 39% by acquired morbidity. In 8% of the children the acquired morbidity was related to complications from PICU procedures. Three months after discharge 77% of the children had normal PCPC scores and 31% had normal POPC scores. Conclusions: Our results indicate that PICU survival may be associated with substantial physical sequelae. Structured follow-up research, preferably by multicenter studies, is warranted in PICU survivor
Genetic relatedness of subgingival and buccal Candida dubliniensis isolates in immunocompetent subjects assessed by RAPD-PCR
- Author
- Alcira Cristina Rosa
- Alicia Cuesta
- Almirante B
- Ascioglu S
- Badoc C
- Binolfi A
- Blignaut E
- Cannon RD
- Costa F
- Cristina Adela iovannitti
- Dahlen G
- Diaz-Guerra TM
- Donnelly SM
- Duran EL
- Fotedar R
- Giammanco GM
- Gilfillan GD
- Hellstein J
- Jabra-Rizk MA
- Jabra-Rizk MA
- Jabra-Rizk MA
- Jain P
- Jewtuchowicz VM
- Jewtuchowicz VM
- Jitsurong S
- Kamei K
- Kirkpatrick WR
- Lamster IB
- Lopez-Ribot JL
- Luque AG
- Maria celina Malzone
- Maria lorena Nastri
- Maria Teresa Mujica
- Martinez M
- Meiller TF
- Milan EP
- Montour L
- Patel M
- Pineda G
- Pizzo G
- Pizzo G
- Polacheck I
- Portela MB
- Pujol C
- Reynaud AH
- Samaranayake YH
- Scherer S
- Silva V
- Soll DR
- Song X
- Song X
- Staib P
- Sullivan D
- Sullivan DJ
- Tamura M
- Tintelnot K
- Virginia Marta Jewtuchowicz
- Waltimo TM
- Waltimo TM
- Williams JG
- Publication venue
- CoAction Publishing
- Publication date
- Field of study
Search for CP violation in D+→ϕπ+ and D+s→K0Sπ+ decays
- Author
- Aaij R
- Adeva B
- Adinolfi M
- Adrover C
- Affolder A
- Ajaltouni Z
- Akiba KC
- Albor VF
- Albrecht J
- Alessio F
- Alexander M
- Ali S
- Alkhazov G
- Altarelli MP
- Alvarez AP
- Alves AA
- Amato S
- Amerio S
- Amhis Y
- Anderlini L
- Anderson J
- Andreassen R
- Appleby RB
- Archilli F
- Artamonov A
- Artuso M
- Aslanides E
- Auriemma G
- Bachmann S
- Back JJ
- Baesso C
- Balagura V
- Baldini W
- Barlow RJ
- Barschel C
- Barsuk S
- Barter W
- Bauer T
- Bay A
- Beddow J
- Bedeschi F
- Bediaga I
- Belogurov S
- Belous K
- Belyaev I
- Ben-Haim E
- Benayoun M
- Bencivenni G
- Benson S
- Benton J
- Berezhnoy A
- Bernet R
- Beteta CA
- Bettler M-O
- Bien A
- Bifani S
- Bird T
- Bizzeti A
- Bjørnstad PM
- Blake T
- Blanc F
- Blouw J
- Blusk S
- Bocci V
- Bondar A
- Bondar N
- Bonivento W
- Borghi S
- Borgia A
- Bowcock TJV
- Bowen E
- Bozzi C
- Brambach T
- Bressieux J
- Brett D
- Britsch M
- Britton T
- Brook NH
- Brown H
- Burducea I
- Bursche A
- Busetto G
- Buytaert J
- Cadeddu S
- Callot O
- Calvi M
- Camboni A
- Campana P
- Carbone A
- Carboni G
- Cardinale R
- Cardini A
- Cardoso LAG
- Carranza-Mejia H
- Carson L
- Cartelle PA
- Casasus MP
- Casse G
- Cattaneo M
- Cauet C
- Charles M
- Charpentier P
- Chen P
- Chiapolini N
- Chrzaszcz M
- Ciba K
- Ciezarek G
- Clarke PEL
- Clemencic M
- Cliff HV
- Closier J
- Coca C
- Coco V
- Cogan J
- Cogneras E
- Collins P
- Comerma-Montells A
- Contu A
- Cook A
- Coombes M
- Coquereau S
- Corti G
- Coutinho RS
- Couturier B
- Cowan GA
- Craik D
- Cunliffe S
- Currie R
- David P
- David PNY
- De Bonis I
- De Bruyn K
- De Capua S
- De Cian M
- De Miranda JM
- De Oyanguren Campos M
- De Paula L
- De Silva W
- De Simone P
- Decamp D
- Deckenhoff M
- Del Buono L
- Derkach D
- Deschamps O
- Dettori F
- Di Canto A
- Diaz RG
- Dijkstra H
- Dogaru M
- Donleavy S
- Dordei F
- dos Reis AC
- Dossett D
- Dovbnya A
- Dupertuis F
- Dzhelyadin R
- Dziurda A
- Dzyuba A
- D’Ambrosio C
- Easo S
- Egede U
- Egorychev V
- Eidelman S
- Eisenhardt S
- Eitschberger U
- Ekelhof R
- Eklund L
- El Rifai I
- Elsasser C
- Elsby D
- Falabella A
- Fardell G
- Farinelli C
- Farry S
- Fave V
- Ferguson D
- Ferro-Luzzi M
- Filippov S
- Fitzpatrick C
- Fontana M
- Fontanelli F
- Forty R
- Francisco O
- Frank M
- Frei C
- Frosini M
- Furcas S
- Furfaro E
- Färber C
- Galli D
- Gandelman M
- Gandini P
- Gao Y
- Garofoli J
- Garosi P
- Garrido L
- Gaspar C
- Gauld R
- Gersabeck E
- Gersabeck M
- Gershon T
- Ghez P
- Gibson V
- Gioi LL
- Gligorov VV
- Goicochea JMO
- Golubkov D
- Golutvin A
- Gomes A
- Gomez MC
- Gordon H
- Graugés E
- Graziani G
- Grecu A
- Greening E
- Gregson S
- Grünberg O
- Gui B
- Gushchin E
- Gutierrez OA
- Guz Y
- Gys T
- Gándara MG
- Göbel C
- Hadjivasiliou C
- Haefeli G
- Haen C
- Haines SC
- Hall S
- Hampson T
- Hansmann-Menzemer S
- Harnew N
- Harnew ST
- Harrison J
- Hartmann T
- He J
- Heijne V
- Hennessy K
- Henrard P
- Hicks E
- Hill D
- Hoballah M
- Hombach C
- Hopchev P
- Hulsbergen W
- Hunt P
- Huse T
- Hussain N
- Hutchcroft D
- Hynds D
- Iakovenko V
- Idzik M
- Ilten P
- Jacobsson R
- Jaeger A
- Jans E
- Jaton P
- Jing F
- John M
- Johnson D
- Jones CR
- Jost B
- Kaballo M
- Kandybei S
- Karacson M
- Karbach TM
- Kenyon IR
- Kerzel U
- Ketel T
- Keune A
- Khanji B
- Kochebina O
- Komarov I
- Koopman RF
- Koppenburg P
- Korolev M
- Kozlinskiy A
- Kravchuk L
- Kreplin K
- Kreps M
- Krocker G
- Krokovny P
- Kruse F
- Kucharczyk M
- Kudryavtsev V
- Kvaratskheliya T
- La Thi VN
- Lacarrere D
- Lafferty G
- Lai A
- Lambert D
- Lambert RW
- Lanciotti E
- Lanfranchi G
- Langenbruch C
- Latham T
- Lazzeroni C
- Le Gac R
- Lees J-P
- Leflat A
- Lefrançois J
- Lefèvre R
- Leo S
- Leroy O
- Leverington B
- Li Y
- Liles M
- Lindner R
- Linn C
- Liu B
- Liu G
- Lohn S
- Lopes JH
- Lopez Asamar E
- Lopez-March N
- Lu H
- Lucchesi D
- Luisier J
- Luo H
- Machefert F
- Machikhiliyan IV
- Maciuc F
- Maev O
- Malde S
- Manca G
- Mancinelli G
- Marconi U
- Marks J
- Martellotti G
- Martens A
- Martin L
- Martinelli M
- Massafferri A
- Matev R
- Mathe Z
- Matteuzzi C
- Maurice E
- Mazurov A
- McCarthy J
- Mcnab A
- McNulty R
- Meadows B
- Meier F
- Meissner M
- Merk M
- Milanes DA
- Minard M-N
- Molina VR
- Monteil S
- Moran D
- Morata JAH
- Morawski P
- Morello MJ
- Mountain R
- Mous I
- Muheim F
- Muresan R
- Muryn B
- Muster B
- Märki R
- Müller K
- Naik P
- Nakada T
- Nandakumar R
- Nasteva I
- Needham M
- Neufeld N
- Nguyen AD
- Nguyen TD
- Nguyen-Mau C
- Nicol M
- Niess V
- Niet R
- Nikitin N
- Nikodem T
- Nomerotski A
- Novoselov A
- Oblakowska-Mucha A
- Obraztsov V
- Oggero S
- Ogilvy S
- Okhrimenko O
- Oldeman R
- Orlandea M
- Owen P
- Pal BK
- Palano A
- Palutan M
- Panman J
- Papanestis A
- Pappagallo M
- Parkes C
- Parkinson CJ
- Passaleva G
- Patel GD
- Patel M
- Patrick GN
- Patrignani C
- Pavel-Nicorescu C
- Pellegrino A
- Penso G
- Perazzini S
- Perego DL
- Perez Trigo E
- Perret P
- Perrin-Terrin M
- Pessina G
- Petridis K
- Petrolini A
- Phan A
- Picatoste Olloqui E
- Pietrzyk B
- Pilař T
- Pinci D
- Playfer S
- Polci F
- Polok G
- Poluektov A
- Polycarpo E
- Popov D
- Popovici B
- Potterat C
- Powell A
- Prisciandaro J
- Pugatch V
- Puig Navarro A
- Punzi G
- Qian W
- Rademacker JH
- Rakotomiaramanana B
- Rangel MS
- Raniuk I
- Rauschmayr N
- Raven G
- Redford S
- Reid MM
- Ricciardi S
- Richards A
- Rinnert K
- Roa Romero DA
- Robbe P
- Rodrigues E
- Rodrigues FF
- Rodriguez Perez P
- Rodriguez JM
- Roiser S
- Romanovsky V
- Romero Vidal A
- Rouvinet J
- Ruf T
- Ruffini F
- Ruiz Valls P
- Ruiz H
- Sabatino G
- Saborido Silva JJ
- Sagidova N
- Sail P
- Saitta B
- Salzmann C
- Sanmartin Sedes B
- Sannino M
- Santacesaria R
- Santamarina Rios C
- Santos DM
- Santovetti E
- Sapunov M
- Sarti A
- Satriano C
- Satta A
- Savrie M
- Savrina D
- Schaack P
- Schiller M
- Schindler H
- Schlupp M
- Schmelling M
- Schmidt B
- Schneider O
- Schopper A
- Schune M-H
- Schwemmer R
- Sciascia B
- Sciubba A
- Seco M
- Semennikov A
- Senderowska K
- Sepp I
- Serra N
- Serrano J
- Seyfert P
- Shapkin M
- Shapoval I
- Shatalov P
- Shcheglov Y
- Shears T
- Shekhtman L
- Shevchenko O
- Shevchenko V
- Shires A
- Skwarnicki T
- Smith E
- Smith M
- Smith NA
- Sokoloff MD
- Soler FJP
- Soomro F
- Souza De Paula B
- Souza D
- Spaan B
- Sparkes A
- Spradlin P
- Stagni F
- Stahl S
- Steinkamp O
- Stoica S
- Stone S
- Storaci B
- Straticiuc M
- Straumann U
- Subbiah VK
- Suárez AD
- Swientek S
- Syropoulos V
- Szczekowski M
- Szczypka P
- Szumlak T
- Sánchez AM
- Teklishyn M
- Teodorescu E
- Teubert F
- The LHCb collaboration
- Thomas C
- Thomas E
- Tico JG
- Tisserand V
- Tobin M
- Tolk S
- Tonelli D
- Topp-Joergensen S
- Torr N
- Torreira AG
- Tostes DM
- Tournefier E
- Tourneur S
- Tran MT
- Tresch M
- Tsaregorodtsev A
- Tsopelas P
- Tuning N
- T’Jampens S
- Ubeda Garcia M
- Ukleja A
- Urner D
- Uwer U
- Vagnoni V
- Valenti G
- van Beuzekom M
- van den Brand J
- van Eijk D
- van Herwijnen E
- van Leerdam J
- van Tilburg J
- Vazquez Gomez R
- Vazquez Regueiro P
- Vecchi S
- Velthuis JJ
- Veltri M
- Veneziano G
- Vesterinen M
- Viaud B
- Vidal XC
- Vieira D
- Vilasis-Cardona X
- Vollhardt A
- Volyanskyy D
- von Loeben J
- Voong D
- Vorobyev A
- Vorobyev V
- Voss H
- Voß C
- Waldi R
- Wallace R
- Wandernoth S
- Wang J
- Ward DR
- Watson NK
- Webber AD
- Websdale D
- Whitehead M
- Wicht J
- Wiechczynski J
- Wiedner D
- Wiggers L
- Wilkinson G
- Williams M
- Williams MP
- Wilson FF
- Wishahi J
- Witek M
- Wotton SA
- Wright S
- Wu S
- Wyllie K
- Xie Y
- Xing F
- Xing Z
- Yang Z
- Young R
- Yuan X
- Yushchenko O
- Yzquierdo AP-C
- Zangoli M
- Zavertyaev M
- Zhang F
- Zhang L
- Zhang WC
- Zhang Y
- Zhelezov A
- Zhokhov A
- Zhong L
- Zvyagin A
- Publication venue
- Springer
- Publication date
- 01/01/2013
- Field of study
A search for CP violation in D + → ϕπ + decays is performed using data collected in 2011 by the LHCb experiment corresponding to an integrated luminosity of 1.0 fb−1 at a centre of mass energy of 7 TeV. The CP -violating asymmetry is measured to be (−0.04 ± 0.14 ± 0.14)% for candidates with K − K + mass within 20 MeV/c 2 of the ϕ meson mass. A search for a CP -violating asymmetry that varies across the ϕ mass region of the D + → K − K + π + Dalitz plot is also performed, and no evidence for CP violation is found. In addition, the CP asymmetry in the D+s→K0Sπ+ decay is measured to be (0.61 ± 0.83 ± 0.14)%
Differential branching fraction and angular analysis of Λb0→Λμ+μ− decays
- Author
- R. Aaij
- B. Adeva
- M. Adinolfi
- A. Affolder
- Z. Ajaltouni
- S. Akar
- J. Albrecht
- F. Alessio
- M. Alexander
- S. Ali
- G. Alkhazov
- P. Alvarez Cartelle
- A. A. Alves
- S. Amato
- S. Amerio
- Y. Amhis
- L. An
- L. Anderlini
- J. Anderson
- M. Andreotti
- J. E. Andrews
- R. B. Appleby
- O. Aquines Gutierrez
- F. Archilli
- A. Artamonov
- M. Artuso
- E. Aslanides
- G. Auriemma
- M. Baalouch
- S. Bachmann
- J. J. Back
- A. Badalov
- C. Baesso
- W. Baldini
- R. J. Barlow
- C. Barschel
- S. Barsuk
- W. Barter
- V. Batozskaya
- V. Battista
- A. Bay
- L. Beaucourt
- J. Beddow
- F. Bedeschi
- I. Bediaga
- L. J. Bel
- I. Belyaev
- E. Ben-Haim
- G. Bencivenni
- S. Benson
- J. Benton
- A. Berezhnoy
- R. Bernet
- A. Bertolin
- M.-O. Bettler
- M. van Beuzekom
- A. Bien
- S. Bifani
- T. Bird
- A. Bizzeti
- T. Blake
- F. Blanc
- J. Blouw
- S. Blusk
- V. Bocci
- A. Bondar
- N. Bondar
- W. Bonivento
- S. Borghi
- M. Borsato
- T. J. V. Bowcock
- E. Bowen
- C. Bozzi
- S. Braun
- D. Brett
- M. Britsch
- T. Britton
- J. Brodzicka
- N. H. Brook
- A. Bursche
- J. Buytaert
- S. Cadeddu
- R. Calabrese
- M. Calvi
- M. Calvo Gomez
- P. Campana
- D. Campora Perez
- L. Capriotti
- A. Carbone
- G. Carboni
- R. Cardinale
- A. Cardini
- P. Carniti
- L. Carson
- K. Carvalho Akiba
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- M. Charles
- Ph. Charpentier
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- S. Chen
- S.-F. Cheung
- N. Chiapolini
- M. Chrzaszcz
- X. Cid Vidal
- G. Ciezarek
- P. E. L. Clarke
- M. Clemencic
- H. V. Cliff
- J. Closier
- V. Coco
- J. Cogan
- E. Cogneras
- V. Cogoni
- L. Cojocariu
- G. Collazuol
- P. Collins
- A. Comerma-Montells
- A. Contu
- A. Cook
- M. Coombes
- S. Coquereau
- G. Corti
- M. Corvo
- I. Counts
- B. Couturier
- G. A. Cowan
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- D. Decamp
- M. Deckenhoff
- L. Del Buono
- N. Déléage
- D. Derkach
- O. Deschamps
- F. Dettori
- B. Dey
- A. Di Canto
- F. Di Ruscio
- H. Dijkstra
- S. Donleavy
- F. Dordei
- M. Dorigo
- A. Dosil Suárez
- D. Dossett
- A. Dovbnya
- K. Dreimanis
- G. Dujany
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- P. Durante
- R. Dzhelyadin
- A. Dziurda
- A. Dzyuba
- S. Easo
- U. Egede
- V. Egorychev
- S. Eidelman
- S. Eisenhardt
- U. Eitschberger
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- C. Frei
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- J. Fu
- E. Furfaro
- A. Gallas Torreira
- D. Galli
- S. Gallorini
- S. Gambetta
- M. Gandelman
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- Y. Gao
- J. García Pardiñas
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- L. A. Granado Cardoso
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- E. Greening
- S. Gregson
- P. Griffith
- L. Grillo
- O. Grünberg
- B. Gui
- E. Gushchin
- Yu. Guz
- T. Gys
- C. Hadjivasiliou
- G. Haefeli
- C. Haen
- S. C. Haines
- S. Hall
- B. Hamilton
- T. Hampson
- X. Han
- S. Hansmann-Menzemer
- N. Harnew
- S. T. Harnew
- J. Harrison
- J. He
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- V. Heijne
- K. Hennessy
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- L. Henry
- J. A. Hernando Morata
- E. van Herwijnen
- M. Heß
- A. Hicheur
- D. Hill
- M. Hoballah
- C. Hombach
- W. Hulsbergen
- T. Humair
- N. Hussain
- D. Hutchcroft
- D. Hynds
- M. Idzik
- P. Ilten
- R. Jacobsson
- A. Jaeger
- J. Jalocha
- E. Jans
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- D. Johnson
- C. R. Jones
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- B. Jost
- N. Jurik
- S. Kandybei
- W. Kanso
- M. Karacson
- T. M. Karbach
- S. Karodia
- M. Kelsey
- I. R. Kenyon
- M. Kenzie
- T. Ketel
- B. Khanji
- C. Khurewathanakul
- S. Klaver
- K. Klimaszewski
- O. Kochebina
- M. Kolpin
- I. Komarov
- R. F. Koopman
- P. Koppenburg
- M. Korolev
- L. Kravchuk
- K. Kreplin
- M. Kreps
- G. Krocker
- P. Krokovny
- F. Kruse
- W. Kucewicz
- M. Kucharczyk
- V. Kudryavtsev
- K. Kurek
- T. Kvaratskheliya
- V. N. La Thi
- D. Lacarrere
- G. Lafferty
- A. Lai
- D. Lambert
- R. W. Lambert
- G. Lanfranchi
- C. Langenbruch
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- F. F. Wilson
- J. Wimberley
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- W. Wislicki
- M. Witek
- G. Wormser
- S. A. Wotton
- S. Wright
- K. Wyllie
- Y. Xie
- Z. Xu
- Z. Yang
- X. Yuan
- O. Yushchenko
- M. Zangoli
- M. Zavertyaev
- L. Zhang
- Y. Zhang
- A. Zhelezov
- A. Zhokhov
- L. Zhong
- T Mannel
- G Hiller
- P Böer
- MJ Aslam
- Y-M Wang
- C-S Huang
- C-H Chen
- C-H Chen
- C-H Chen
- F Zolfagharpour
- L Mott
- TM Aliev
- R Mohanta
- S Sahoo
- W Detmold
- T Gutsche
- M Beylich
- M Beneke
- T Sjöstrand
- DJ Lange
- P Golonka
- AJ Buras
- AJ Buras
- WD Hulsbergen
- M Feindt
- TM Aliev
- S Descotes-Genon
- GJ Feldman
- B Sen
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2003
- Field of study
The differential branching fraction of the rare decay Λb0→Λμ+μ− is measured as a function of q2, the
square of the dimuon invariant mass. The analysis is performed using
proton-proton collision data, corresponding to an integrated luminosity of 3.0
\mbox{ fb}^{-1}, collected by the LHCb experiment. Evidence of signal is
observed in the q2 region below the square of the J/ψ mass. Integrating
over 15 < q^{2} < 20 \mbox{ GeV}^2/c^4 the branching fraction is measured as
d\mathcal{B}(\Lambda^{0}_{b} \rightarrow \Lambda \mu^+\mu^-)/dq^2 = (1.18 ^{+
0.09} _{-0.08} \pm 0.03 \pm 0.27) \times 10^{-7} ( \mbox{GeV}^{2}/c^{4})^{-1},
where the uncertainties are statistical, systematic and due to the
normalisation mode, Λb0→J/ψΛ, respectively.
In the q2 intervals where the signal is observed, angular distributions are
studied and the forward-backward asymmetries in the dimuon (AFBl)
and hadron (AFBh) systems are measured for the first time. In the
range 15 < q^2 < 20 \mbox{ GeV}^2/c^4 they are found to be A^{l}_{\rm FB} =
-0.05 \pm 0.09 \mbox{ (stat)} \pm 0.03 \mbox{ (syst)} and A^{h}_{\rm FB} =
-0.29 \pm 0.07 \mbox{ (stat)} \pm 0.03 \mbox{ (syst)}.Comment: 27 pages, 10 figures, Erratum adde
Effective Rheology of Bubbles Moving in a Capillary Tube
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- Adam J
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- Zetina LM
- Zgura IS
- Zhalov M
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- 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
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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- Zhemchugov A
- Zheng Z
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- 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
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
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- Yang H
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- 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
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- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- 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
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
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- Abdallah J
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- Zurzolo G
- Zutshi V
- Zwalinski L
- 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
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
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- Esposito B
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- Etienne F
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- Etienvre AI
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- Etzion E
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- Evans H
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- Fabbri L
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- Farrell S
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- Farthouat P
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- Favareto A
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- Fedorko W
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- Feigl S
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- Feligioni L
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- Feng C
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- Flowerdew MJ
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- Formica A
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- Forti A
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- Wotschack J
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- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √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 pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
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- Youssef S
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- Zaidan R
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- Zanzi D
- Zeitnitz C
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- Zemla A
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
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