999 research outputs found
Lattice Boltzmann simulations of soft matter systems
- Author
- A Alexeev
- A Chatterji
- A Chatterji
- A Levine
- A Malevanets
- A Malevanets
- A Ricci
- A Sierou
- AG Schlijper
- AJ Banchio
- AJ Wagner
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AJC Ladd
- AK Gunstensen
- AS Sangani
- AY Grosberg
- B Chun
- B Chun
- B Cichocki
- B Cichocki
- B Cichocki
- B Dünweg
- B Dünweg
- B Dünweg
- B Dünweg
- B Liu
- B Wachmann
- BH Zimm
- BJ Alder
- BM Boghosian
- BP Ho
- C Junghans
- C Pierleoni
- CK Aidun
- CK Ghadder
- CP Lowe
- CS Peskin
- CW Gardiner
- CWJ Beenakker
- D D'Humières
- D D'Humières
- D Long
- D Richter
- D Saintillan
- DA Weitz
- DF Evans
- DL Ermak
- DL Koch
- DP Landau
- E Guazzelli
- E Herbolzheimer
- E Wajnryb
- EH Hauge
- EJ Ding
- EJ Hinch
- EJ Hinch
- ES Asmolov
- F Higuera
- F Thalmann
- FJ Alexander
- G Besold
- G Bussi
- G Giupponi
- G Gonnella
- G Segré
- GA Buxton
- GD Fabritiis
- GD Fabritiis
- GR McNamara
- GR McNamara
- GR McNamara
- GS Grest
- H Hasimoto
- H Ma
- H Nicolai
- H Risken
- HA Forbert
- HC Öttinger
- HD Chen
- HD Chen
- I Ginzburg
- I Ginzburg
- I Halliday
- I Pagonabarraga
- I Vattulainen
- IL Claeys
- IV Karlin
- J Happel
- J Lyklema
- J Matas
- J Rotne
- J Zheng
- J Zheng
- JA Schonberg
- JB Gibson
- JD Weeks
- JE Butler
- JF Brady
- JF Brady
- JHC Luke
- JMVA Koelman
- JP Hansen
- JP Hernande-Ortiz
- JP Matas
- JR Blake
- JR Dorfman
- JX Zhu
- K Höfler
- K Mussawisade
- L Fang
- LD Landau
- LS Luo
- LS Luo
- M Bouzidi
- M Doi
- M Fixman
- M Frank
- M Junk
- M Kröger
- M Serrano
- MA Hoef van der
- MA Hoef van der
- MG Fyta
- MH Ernst
- MH Kao
- MP Brenner
- MR Maxey
- MR Swift
- N Kikuchi
- N Liron
- N Sharma
- NA Spenley
- NI Prasianakis
- NQ Nguyen
- O Filippova
- OB Usta
- OB Usta
- OB Usta
- P Ahlrichs
- P Ahlrichs
- P Ahlrichs
- P Español
- P Español
- P Español
- P Lallemand
- P Lallemand
- P Lallemand
- P Mazur
- P Nelson
- P Nikunen
- P Tong
- PE Rouse
- PG Gennes de
- PG Gennes de
- PG Saffman
- PJ Hoogerbrugge
- PJ Mucha
- PM Chaikin
- Q Li
- Q Meng
- Q Meng
- R Adhikari
- R Benzi
- R Car
- R Delgad-Buscalioni
- R Delgad-Buscalioni
- R Delgad-Buscalioni
- R Delgad-Buscalioni
- R Groot
- RB Bird
- RE Caflisch
- RF Fox
- RI McLachlan
- RM Jendrejack
- RM Jendrejack
- RM Jendrejack
- RW Mei
- RW Nash
- S Ansumali
- S Arcidiacono
- S Chandrasekhar
- S Chapman
- S Lomholt
- S Schwarzer
- S Succi
- T Ihle
- T Ihle
- T Ihle
- T Ihle
- T Shardlow
- T Soddemann
- U Frisch
- U Frisch
- V Lobaskin
- V Lobaskin
- V Lobaskin
- VE Zakharov
- W Gunsteren van
- W Kalthoff
- W Montfrooij
- W Smith
- WB Russel
- X Shan
- X Shi
- YH Qian
- Z Guo
- Z Guo
- Z Guo
- ZG Feng
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2008
- Field of study
This article concerns numerical simulations of the dynamics of particles
immersed in a continuum solvent. As prototypical systems, we consider colloidal
dispersions of spherical particles and solutions of uncharged polymers. After a
brief explanation of the concept of hydrodynamic interactions, we give a
general overview over the various simulation methods that have been developed
to cope with the resulting computational problems. We then focus on the
approach we have developed, which couples a system of particles to a lattice
Boltzmann model representing the solvent degrees of freedom. The standard D3Q19
lattice Boltzmann model is derived and explained in depth, followed by a
detailed discussion of complementary methods for the coupling of solvent and
solute. Colloidal dispersions are best described in terms of extended particles
with appropriate boundary conditions at the surfaces, while particles with
internal degrees of freedom are easier to simulate as an arrangement of mass
points with frictional coupling to the solvent. In both cases, particular care
has been taken to simulate thermal fluctuations in a consistent way. The
usefulness of this methodology is illustrated by studies from our own research,
where the dynamics of colloidal and polymeric systems has been investigated in
both equilibrium and nonequilibrium situations.Comment: Review article, submitted to Advances in Polymer Science. 16 figures,
76 page
Segmental resection of the duodenum for gastrointestinal stromal tumor (GIST)
- Author
- B Nilsson
- Bernd Schulte
- BK Goh
- BK Goh
- C Stratopoulos
- CD Fletcher
- CL Corless
- D Hompes
- DK Filippou
- Friedrich W Pelster
- GD Demetri
- H Joensuu
- H Uchida
- Heiner H Wolters
- I Pidhorecky
- K Uehara
- LG Kindblom
- M Cavallini
- M Chiarugi
- M Miettinen
- M Sarlomo-Rikala
- MT Mazur
- N Kurihara
- P De Nicola
- RD Winfield
- Rudolf Mennigen
- S Hinz
- S Hirota
- SH Kwon
- T Aparicio
- T Tran
- WG Goettsch
- Y Fujimoto
- Y Sakamoto
- Publication venue
- BioMed Central
- Publication date
- 01/01/2008
- Field of study
<p>Abstract</p> <p>Background</p> <p>Gastrointestinal stromal tumors (GIST) are the most frequent mesenchymal tumors of the gastrointestinal tract. The biological appearance of these tumors reaches from small lesions with benign appearance to aggressive sarcomas. Only 3–5% of GISTs are localized in the duodenum. There is a controversy, if duodenal GISTs should be treated by a duodenopancreatectomy or by a limited resection of the duodenum.</p> <p>Case presentation</p> <p>A 29-year-old man presented with an acute upper gastrointestinal bleeding from a submucosal tumor located in the proximal part III of the duodenum, 3 cm distal of the papilla of Vater. After an emergency laparotomy with ligation of tumor-feeding vessels in a primary hospital, definitive surgical therapy was performed by partial resection of the duodenum with a duodenojejunostomy. Histology revealed a GIST with a diameter of 2.5 cm and <5 mitoses/50 high power fields, indicating a low risk of malignancy. Therefore no adjuvant therapy with Imatinib was initiated.</p> <p>Conclusion</p> <p>GISTs of the duodenum are a rare cause of upper gastrointestinal bleeding. Partial resection of the duodenum is a warranted alternative to a duodenopancreatectomy, as this procedure has a lower operative morbidity, while providing comparable oncological results.</p
Malignant gastrointestinal stromal tumor presenting with hemoperitoneum in puerperium: report of a case with review of the literature
- Author
- AT Van Oosterom
- CBM Wingen
- Ch Akrivis
- Christodoulos Akrivis
- E Towu
- Evangelia Skafida
- GD Demetri
- GR Nigri
- H Joensuu
- H Maeda
- H Marret
- I Zighelboim
- JA Crosby
- JJ Lewis
- JL Powell
- K Kitabayashi
- K Nasu
- L Thomsen
- LG Kindblom
- M Miettinen
- M Takano
- M Varras
- MC Renaud
- Michail Varras
- MT Mazur
- Nikolaos Vlachakos
- PT Valente
- S Erkanli
- S Hirota
- S Hsu
- S Lanzafame
- S Scherjon
- T Ueyama
- Thivi Vasilakaki
- WM Klein
- Y Morimura
- YK Cheon
- Z Belics
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
Search for rare quark-annihilation decays, B --> Ds(*) Phi
- Author
- Abe T
- Abrams GS
- Adye T
- Ahmed M
- Ahmed S
- Alam MS
- Albert J
- Aleksan R
- Allen MT
- Allison J
- Allmendinger T
- Altenburg D
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Aston D
- Aubert B
- Azzolini V
- Baak M
- Back JJ
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Barate R
- Bard DJ
- Barlow NR
- Barlow RJ
- Barrett M
- Bartoldus R
- Batignani G
- Battaglia M
- Bauer JM
- Beck TW
- Behera PK
- Bellini F
- Benayoun M
- Benelli G
- Berger N
- Bernard D
- Berryhill JW
- Best D
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhimji W
- Bhuyan B
- Bianchi F
- Biasini M
- Biesiada J
- Blanc F
- Blaylock G
- Blinov AE
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bona M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandenburg G
- Brandt T
- Brau J
- Breon AB
- Brose J
- Brown CL
- Brown CM
- Brown DN
- Brown DN
- Bruinsma M
- Brunet S
- Bucci F
- Buchanan C
- Buchmueller OL
- Bugg W
- Bukin AD
- Bula R
- Bulten H
- Buono LD
- Burchat PR
- Burke JP
- Button-Shafer J
- Buzzo A
- Cahn RN
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Capra R
- Carpinelli M
- Cartaro C
- Cavallo N
- Cavoto G
- Cenci R
- Chai X
- Chaisanguanthum KS
- Chao M
- Charles E
- Charles MJ
- Chauveau J
- Chavez CA
- Chen A
- Chen C
- Chen E
- Chen JC
- Chen S
- Chen X
- Cheng B
- Cheng CH
- Chia YM
- Cibinetto G
- Clark PJ
- Claus R
- Cochran J
- Coleman JP
- Collaboration BABAR
- Contri R
- Convery MR
- Cossutti F
- Cote D
- Cottingham WN
- Couderc F
- Covarelli R
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Cristinziani M
- Cuhadar-Donszelmann T
- Cunha A
- Curry S
- D'Orazio A
- Dahmes B
- Dallapiccola C
- Danielson N
- Dasu S
- Datta M
- Dauncey PD
- David P
- Davier M
- Davis CL
- Day CT
- de la Vaissiere C
- de Monchenault GH
- de Sangro R
- del Re D
- Diberder FL
- Dickopp M
- Dingfelder JC
- Dittongo S
- Dong D
- Dong L
- Dorfan J
- Druzhinin VP
- Dubitzky RS
- Dubois-Felsmann GP
- Dujmic D
- Dunwoodie W
- Dvoretskii A
- Eckhart EA
- Eckmann R
- Edgar CL
- Edwards AJ
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
- Emery S
- Ernst JA
- Eschenburg V
- Eschrich I
- Eyges V
- Fabozzi F
- Faccini R
- Fan S
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Flacco CJ
- Flack RL
- Flaecher HU
- Flood KT
- Ford KE
- Ford WT
- Forster IJ
- Forti F
- Fortin D
- Foulkes SD
- Franek B
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabathuler E
- Gaidot A
- Gaillard JR
- Galeazzi F
- Gallo F
- Gamba D
- Gamet R
- Gan KK
- Ganzhur SF
- Gary JW
- Gaspero M
- Gatto C
- George KA
- Gill MS
- Gioi LL
- Giorgi MA
- Giroux X
- Gladney L
- Glanzman T
- Godang R
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy SJ
- Gradl W
- Graham MT
- Grancagnolo S
- Grauges E
- Graziani G
- Green MG
- Grenier P
- Gritsan AV
- Groot ND
- Grosdidier G
- Groysman Y
- Guo QH
- Hadavand HK
- Hadig T
- Haire M
- Halyo V
- Hamano K
- Hamon O
- Harrison PF
- Harrison TJ
- Hart AJ
- Hartfiel BL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Held T
- Hertzbach SS
- Heusch CA
- Hill EJ
- Hirschauer JF
- Hitlin DG
- Hocker A
- Hodgkinson MC
- Hollar JJ
- Hong TM
- Honscheid K
- Hopkins DA
- Hryn'ova T
- Hufnagel D
- Hulsbergen WD
- Hutchcroft DE
- Igonkina O
- Innes WR
- Izen JM
- Jackson PD
- Jackson PS
- Jacobsen RG
- Jawahery A
- Jessop CP
- John MJJ
- Johnson JR
- Judd D
- Kadel RW
- Kadyk J
- Kagan H
- Karyotakis Y
- Kass R
- Kelly MP
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
- Kim P
- Kirkby D
- Kitayama I
- Klose V
- Knecht NS
- Koch H
- Kocian ML
- Koeneke K
- Kofler R
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kozanecki W
- Kravchenko EA
- Kreisel A
- Krishnamurthy M
- Kroeger R
- Kroseberg J
- Kukartsev G
- Kutter PE
- Kyberd P
- Lacker HM
- Lae CK
- Lafferty GD
- Lanceri L
- Lange DJ
- Langenegger U
- Lankford AJ
- Latham TE
- Latour E
- Lau YP
- Lazzaro A
- Lees JP
- Legendre M
- Leith DWGS
- Lepeltier V
- Leruste P
- Lewandowski B
- Li H
- Li X
- Libby J
- Lista L
- Liu R
- Lockman WS
- Lodovico FD
- Lombardo V
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu C
- Lu M
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Macri MM
- Mader WF
- Majewski SA
- Malcles J
- Mallik U
- Mancinelli G
- Mandelkern M
- Marchiori G
- Marco ED
- Margoni M
- Marks J
- Marsiske H
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazur MA
- Mazzoni MA
- McKenna JA
- McMahon TR
- Meadows BT
- Mellado B
- Menges W
- Messner R
- Meyer WT
- Mihalyi A
- Minamora JS
- Mir LM
- Mohanty GB
- Mohapatra AK
- Mommsen RK
- Monge MR
- Monorchio D
- Moore TB
- Morandin M
- Morgan SE
- Morganti M
- Morganti S
- Morii M
- Muheim F
- Muller DR
- Naisbit MT
- Nardo GD
- Narsky I
- Nash JA
- Nauenberg U
- Neal H
- Negrini M
- Neri N
- Nesom G
- Nicholson H
- Nikolich MB
- Nogowski R
- Nugent IM
- O'Grady CP
- Ocariz J
- Oddone PJ
- Ofte I
- Olaiya EO
- Olivas A
- Olsen J
- Onuchin AP
- Orimoto TJ
- Otto S
- Oyanguren A
- Ozcan VE
- Paar HP
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Pappagallo M
- Parry RJ
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pelizaeus M
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petersen BA
- Petersen TC
- Petzold A
- Piatenko T
- Piccolo D
- Piccolo M
- Piemontese L
- Pierini M
- Pioppi M
- Piredda G
- Plaszczynski S
- Playfer S
- Poireau V
- Polci F
- Pompili A
- Porter FC
- Posocco M
- Potter CT
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Rahatlou S
- Rahimi AM
- Rahmat R
- Rama M
- Ratcliff BN
- Raven G
- Reidy J
- Ricca GD
- Ricciardi S
- Richman JD
- Ritchie JL
- Rizzo G
- Roat C
- Roberts DA
- Robertson SH
- Robutti E
- Rodier S
- Roe NA
- Roethel W
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roudeau P
- Rubin AE
- Ruddick WO
- Ryd A
- Sacco R
- Saeed MA
- Saleem M
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Santroni A
- Saremi S
- Satpathy A
- Schalk T
- Schenk S
- Schindler RH
- Schofield KC
- Schott G
- Schrenk S
- Schroder H
- Schroeder T
- Schubert J
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Serednyakov SI
- Sharma V
- Shen BC
- Simi G
- Simonetto F
- Sinev NB
- Skovpen YI
- Smith AJS
- Smith JG
- Snoek HL
- Snyder A
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Spaan B
- Spanier SM
- Spitznagel M
- Spradlin P
- Staengle H
- Steinke M
- Stelzer J
- Stocchi A
- Stoker DP
- Stroili R
- Strom D
- Strube J
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sundermann JE
- Suzuki K
- Swain SK
- Tan P
- Taras P
- Taylor F
- Tehrani FS
- Telnov AV
- Teodorescu L
- Ter-Antonyan R
- Therin G
- Thiebaux C
- Thompson JM
- Tisserand V
- Toki WH
- Torrence E
- Tosi S
- Touramanis C
- Ulmer KA
- Uwer U
- Va'vra J
- van Bakel N
- Vasileiadis G
- Vasseur G
- Vazquez WP
- Verderi M
- Verkerke W
- Vetere ML
- Viaud FB
- Vitale L
- Voci C
- Voena C
- Wagner SR
- Wagoner DE
- Waldi R
- Walsh J
- Wang K
- Wang P
- Wang WF
- Wappler FR
- Watson AT
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams JC
- Willocq SY
- Wilson FF
- Wilson JR
- Wilson MG
- Wilson RJ
- Winklmeier F
- Wisniewski WJ
- Wittgen M
- Wong QK
- Wormser G
- Wright DH
- Wright DM
- Wu J
- Wu SL
- Xie Y
- Yamamoto RK
- Yarritu AK
- Ye S
- Yeche C
- Yi JI
- Yi K
- Young CC
- Yu Z
- Yushkov AN
- Zain SB
- Zallo A
- Zeng Q
- Zghiche A
- Zhang J
- Zhang L
- Zhao HW
- Zhu YS
- Ziegler V
- Zito M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 12/12/2005
- Field of study
We report on searches for B- --> Ds- Phi and B- --> Ds*- Phi. In the context
of the Standard Model, these decays are expected to be highly suppressed since
they proceed through annihilation of the b and u-bar quarks in the B- meson.
Our results are based on 234 million Upsilon(4S) --> B Bbar decays collected
with the BABAR detector at SLAC. We find no evidence for these decays, and we
set Bayesian 90% confidence level upper limits on the branching fractions BF(B-
--> Ds- Phi) Ds*- Phi)<1.2x10^(-5). These results
are consistent with Standard Model expectations.Comment: 8 pages, 3 postscript figues, submitted to Phys. Rev. D (Rapid
Communications
Measurement of the branching fraction and CP content for the decay B(0) -> D(*+)D(*-)
- Author
- Abe K
- Abrams GS
- Adam I
- Adye T
- Albert J
- Aleksan R
- Allison J
- Alsmiller JRG
- Angelini C
- Anjomshoaa A
- Anulli F
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- BABAR Collaboration
- Back JJ
- Bagnasco S
- Baldini-Ferroli R
- Band HR
- Barillari T
- Barlow NR
- Barlow RJ
- Bartoldus R
- Batignani G
- Bauer JM
- Bellodi G
- Benayoun M
- Berger N
- Beringer J
- Bernard D
- Bernet R
- Best D
- Bettarini S
- Bevan AJ
- Bhimji W
- Bianchi F
- Bionta RM
- Blaylock G
- Blinov VE
- Bloom P
- Blouw J
- Bona M
- Bondioli M
- Bonneaud GR
- Borean C
- Borgland AW
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandt T
- Brau B
- Brau J
- Breon AB
- Briand H
- Brigljevic V
- Brochard F
- Brose J
- Brown CM
- Brown D
- Brown DN
- Bucci F
- Buchanan C
- Bugg W
- Bukin AD
- Bukin DA
- Burchat PR
- Button-Shafer J
- Buzykaev AR
- Buzzo A
- Cahn RN
- Calcaterra A
- Calderini G
- Campagna E
- Campagnari C
- Carpinelli M
- Cartaro C
- Cavallo N
- Cavoto G
- Chao M
- Charles E
- Chauveau J
- Chen E
- Chen GP
- Chen JC
- Cheng CH
- Chevalier N
- Christ S
- Chun S
- Clark PJ
- Cochran J
- Cohen-Tanugi J
- Cohn H
- Colberg T
- Colecchia F
- Contri R
- Convery MR
- Cottingham WN
- Coupal DP
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Crosetti G
- Dahmes B
- Dal Corso F
- Dallapiccola C
- Dasu S
- Datta M
- Dauncey PD
- David P
- Davis CL
- De Groot N
- De Nardo G
- de Sangro R
- de Vaissiere C
- Del Buono L
- del Re D
- Della Ricca G
- Deppermann T
- Devmal S
- Di Lodovico F
- Dickopp M
- Dittongo S
- Dixon P
- Dong D
- Dorfan J
- Dorigo A
- Dubitzky RS
- Dubois-Felsmann GP
- Dunwoodie W
- Dvoretskii A
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Emery S
- Eschenburg V
- Eschrich I
- Fabozzi F
- Faccini R
- Falbo M
- Falciai D
- Farbin A
- Ferrag S
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fischer PA
- Flood K
- Ford WT
- Forti AC
- Forti F
- Foster B
- Franek B
- Frank ED
- Frey R
- Fry JR
- Gabathuler E
- Gabriel TA
- Gaidot A
- Gaillard JM
- Galeazzi F
- Gamba D
- Gamet R
- Ganzhur SF
- Gatto C
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- Zito M
- Publication venue
- American Physical Society
- Publication date
- 01/01/2002
- Field of study
This is the pre-print version of the Article. The official published version can be accessed from the links below. Copyright @ 2002 APS.We report a measurement of the branching fraction of the decay B0→D*+D*- and of the CP-odd component of its final state using the BABAR detector. With data corresponding to an integrated luminosity of 20.4 fb-1 collected at the Υ(4S) resonance during 1999–2000, we have reconstructed 38 candidate signal events in the mode B0→D*+D*- with an estimated background of 6.2±0.5 events. From these events, we determine the branching fraction to be B(B0→D*+D*-)=[8.3±1.6(stat)±1.2(syst)]×10-4. The measured CP-odd fraction of the final state is 0.22±0.18(stat)±0.03(syst).This work is supported by DOE and NSF (USA), NSERC (Canada), IHEP (China), CEA and CNRS-IN2P3 (France), BMBF (Germany), INFN (Italy), NFR (Norway), MIST (Russia), and PPARC (United Kingdom). Individuals have received support from the A.P. Sloan Foundation, Research Corporation, and Alexander von Humboldt Foundation
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Abdallah J
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- Yildizb HD
- Yilmaz M
- Yoosootiniya R
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- Zarzhitsky P
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- Zerwas D
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonelli S
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arms KE
- Armstrong SR
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auerbach B
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- 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
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
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
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- Ahlen SP
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- Ahsan M
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- Akesson TPA
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- Aleksandrov IN
- Alessandria F
- Alexa C
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- Alexandre G
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- Alimonti G
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
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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
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
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- 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
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- Aliev M
- Alimonti G
- Alison J
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
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- Alonso A
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- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
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- Anduaga XS
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- Anghinolfi F
- Anisenkov A
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- Asman B
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- Astbury A
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- ATLAS Collaboration The
- Auerbach B
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- Baccaglioni G
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- Zhemchugov A
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- Zmouchko VV
- Zobernig G
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- 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 R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Yamaguchi H
- Yamamoto A
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- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Smit GVY
- Ye J
- Ye S
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
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- Yu J
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- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
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- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou Y
- Zhu CG
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb−1 of s=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan β < 40
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