431 research outputs found
Observation and study of baryonic B decays: B -> D(*) p pbar, D(*) p pbar pi, and D(*) p pbar pi pi
- Author
- Adametz A
- Adye T
- Ahmed S
- Ahmed S
- Alam MS
- Alam MS
- Albert J
- Albert J
- Allen MT
- Alwyn KE
- Anderson J
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Ayad R
- Azzolini V
- Bailey D
- Baldini-Ferroli R
- Band HR
- Band HR
- Banerjee S
- Banerjee S
- Baracchini E
- Bard DJ
- Barlow RJ
- Bartoldus R
- Batignani G
- Battaglia M
- Behera PK
- Bellis M
- Ben-Haim E
- Benitez JF
- Bernard D
- Bernlochner FU
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bhuyan B
- Bianchi F
- Bianchi F
- Biasini M
- Biassoni P
- Bingham I
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bomben M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Bozzi C
- Brau J
- Briand H
- Brown DN
- Brown DN
- Bula R
- Burchat PR
- Burchat PR
- Buzykaev AR
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Cartaro C
- Cartaro C
- Casarosa G
- Castelli G
- Cavoto G
- Cecchi A
- Cenci R
- Cervelli A
- Chauveau J
- Chavez CA
- Chen C
- Chen X
- Chen XR
- Cheng CH
- Choi HHF
- Cibinetto G
- Clark PJ
- Cochranz J
- Coleman JP
- Contri R
- Convery MR
- Corwin LA
- Cossutti F
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Curry S
- da Costa JF
- Dallapiccola C
- Dasu S
- Dasu S
- Dauncey PD
- Davier M
- Davis CL
- de Monchenault GH
- De Nardo G
- de Sangro R
- Della Ricca G
- Denig AG
- Derkach D
- Di Lodovico F
- Doll DA
- Dong L
- Dorfan J
- Druzhinin VP
- Dubois-Felsmann GP
- Dubrovin MS
- Dujmic D
- Dunwoodie W
- Ebert M
- Echenard B
- Eckmann R
- Eckmann R
- Edwards AJ
- Edwards AJ
- Eigen G
- Eisner AM
- Emery S
- Ernst JA
- Ernst JA
- Faccini R
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fioravanti E
- Flanigan JM
- Flood KT
- Flood KT
- Ford WT
- Forti F
- Franchini P
- Franek B
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabareen AM
- Gabathuler E
- Gagliardi N
- Gallo F
- Gamba D
- Gamba D
- Gamet R
- Gary JW
- Gaspero M
- Gaz A
- Gershon TJ
- Gioi LL
- Giorgi MA
- Godang R
- Golubev VB
- Gradl W
- Graham MT
- Grauges E
- Grenier P
- Gritsan AV
- Grosdidier G
- Guido E
- Guo ZJ
- Guttman N
- Hafner A
- Hamano K
- Hamano K
- Hamon O
- Harrison PF
- Harrison PF
- Hartmann T
- Hast C
- Hawkes CM
- Hearty C
- Heusch CA
- Hitlin DG
- Hollar JJ
- Hong TM
- Honscheid K
- Hooberman B
- Hutchcroft DE
- Igonkina O
- Ilic J
- Innes WR
- Izen JM
- Izen JM
- Jackson G
- Jain V
- Jasper H
- Jawahery A
- Jessop CP
- Karbach TM
- Kass R
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
- Kim P
- Kim P
- King GJ
- Kirkby D
- Knoepfel KJ
- Kobel MJ
- Koch H
- Kocian ML
- Kocian ML
- Kolb JA
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kowalewski R
- Krishnamurthy M
- Kroeger R
- Kroseberg J
- Kutter PE
- Lacker HM
- Lafferty GD
- Lanceri L
- Lanceri L
- Lange DJ
- Lankford AJ
- Latham TE
- Latham TE
- Lazzaro A
- Le Diberder F
- Leddig T
- Lee CL
- Lees JP
- Leith DWGS
- Leith DWGS
- Leruste P
- Lewczuk MJ
- Li S
- Li S
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman WS
- Lombardo V
- Long O
- Lopez-March N
- Lopez-March N
- LoSecco JM
- Lou XC
- Lou XC
- Lu C
- Lueck T
- Luitz S
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- Lynch HL
- MacFarlane DB
- MacFarlane DB
- Majewski SA
- Malaescu B
- Mallik U
- Mancinelli G
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Marks J
- Marsiske H
- Marsiske H
- Martin EC
- Martinelli M
- Martinez AJ
- Martinez-Vidal F
- Martinez-Vidal F
- Mattison TS
- Mazzoni MA
- McKenna JA
- Meadows BT
- Merkel J
- Messner R
- Meyer WT
- Milanes DA
- Milanes DA
- Miyashita TS
- Miyashita TS
- Mohanty GB
- Monge MR
- Monorchio D
- Morandin M
- Morii M
- Morris JP
- Muller DR
- Muller DR
- Munerato M
- Nagel M
- Nauenberg U
- Neal H
- Neal H
- Negrini M
- Nelson S
- Neri N
- Nguyen X
- Nicolaci M
- Nugent IM
- Nugent IM
- O'Grady CP
- O'Grady CP
- Ocariz J
- Ofte I
- Ofte I
- Olaiya EO
- Olsen J
- Ongmongkolkul P
- Onorato G
- Onuchin AP
- Osipenkov IL
- Oyanguren A
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan B
- Pan B
- Pan Y
- Pan Y
- Paoloni E
- Pappagallo M
- Paramesvaran S
- Park W
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pegna DL
- Pelliccioni M
- Pelliccioni M
- Perazzo A
- Perez A
- Perl M
- Perl M
- Peruzzi IM
- Petersen BA
- Petrella A
- Petzold A
- Piccolo M
- Piemontese L
- Pierini M
- Piredda G
- Playfer S
- Poireau V
- Porter FC
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prendki J
- Prepost R
- Prepost R
- Puccio EMT
- Pulliam T
- Pulliam T
- Purohit MV
- Rahmat R
- Rakitin AY
- Rama M
- Randle-Conde A
- Ratcliff BN
- Ratcliff BN
- Raven G
- Renga F
- Richman JD
- Ritchie JL
- Ritchie JL
- Rizzo G
- Roberts DA
- Robertson SH
- Robutti E
- Roney JM
- Roney JM
- Roodman A
- Roodman A
- Rosenberg EI
- Rossi A
- Rotondo M
- Roudeau P
- Rubin AE
- Ruland AM
- Ruland AM
- Sacco R
- Saeed MA
- Saeed MA
- Salnikov AA
- Salnikov AA
- Salvati E
- Sanchez PDA
- Santoro V
- Schalk T
- Schilling CJ
- Schilling CJ
- Schindler RH
- Schindler RH
- Schram M
- Schroeder H
- Schroeder T
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwiening J
- Schwierz R
- Schwitters RF
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Serednyakov SI
- Serrano J
- Sevilla MF
- Sigamani M
- Simard M
- Simi G
- Simonetto F
- Sinev NB
- Sitt S
- Skovpen YI
- Smith AJS
- Smith JG
- Snoek HL
- Snyder A
- Snyder A
- Sobie RJ
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Sonnek P
- Sordini V
- Spaan B
- Spanier SM
- Spanier SM
- Stocchi A
- Stoker DP
- Stracka S
- Stroili R
- Strom D
- Strube J
- Stugu B
- Su D
- Su D
- Sullivan MK
- Sullivan MK
- Summers DJ
- Sun L
- Sun S
- Suzuki K
- Suzuki K
- Swain SK
- Tanabe T
- Taras P
- Telnov AV
- Thompson JM
- Thompson JM
- Tibbetts M
- Tico JG
- Tisserand V
- Todyshev KY
- Toki WH
- Torrence E
- Tosi S
- Touramanis C
- Tuggle JM
- Uwer U
- Va'vra J
- Va'vra J
- Vasseur G
- Verderi M
- Vitale L
- Vitale L
- Vitug GM
- Volk A
- Vuosalo CO
- Wacker K
- Wagner AP
- Wagner AP
- Wagner SR
- Waldi R
- Walsh JJ
- Wang L
- Wang WF
- Wappler FR
- Watson AT
- Watson JE
- Weaver M
- Weaver M
- West C
- West CA
- White RM
- Wilden L
- Wilson FF
- Wilson JR
- Wilson P
- Winer BL
- Winstrom LO
- Wisniewski WJ
- Wisniewski WJ
- Wittgen M
- Wittgen M
- Wittich P
- Wolbers S
- Wolfe H
- Wormser G
- Wray BC
- Wren AC
- Wright DH
- Wright DH
- Wright DM
- Wright T
- Wu SL
- Wu SL
- Wu X
- Wu Z
- Wulsin HW
- Yamamoto K
- Yamato D
- Yang T
- Yang UK
- Yang YC
- Yao WM
- Yarritu AK
- Yarritu AK
- Ye S
- Yeche C
- Yeh GP
- Yi K
- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Young CC
- Young CC
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Yushkov AN
- Zain SB
- Zain SB
- Zallo A
- Zanetti A
- Zeng Y
- Zhao M
- Zhou C
- Ziegler V
- Ziegler V
- Zito M
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 15/08/2009
- Field of study
We present a study of ten B-meson decays to a D(*), a proton-antiproton pair,
and a system of up to two pions using BaBar's data set of 455x10^6 BBbar pairs.
Four of the modes (B0bar -> D0 p anti-p, B0bar -> D*0 p anti-p, B0bar -> D+ p
anti-p pi-, B0bar -> D*+ p anti-p pi-) are studied with improved statistics
compared to previous measurements; six of the modes (B- -> D0 p anti-p pi-, B-
-> D*0 p anti-p pi-, B0bar -> D0 p anti-p pi- pi+, B0bar -> D*0 p anti-p pi-
pi+, B- -> D+ p anti-p pi- pi-, B- -> D*+ p anti-p pi- pi-) are first
observations. The branching fractions for 3- and 5-body decays are suppressed
compared to 4-body decays. Kinematic distributions for 3-body decays show
non-overlapping threshold enhancements in m(p anti-p) and m(D(*)0 p) in the
Dalitz plots. For 4-body decays, m(p pi-) mass projections show a narrow peak
with mass and full width of (1497.4 +- 3.0 +- 0.9) MeV/c2, and (47 +- 12 +- 4)
MeV/c2, respectively, where the first (second) errors are statistical
(systematic). For 5-body decays, mass projections are similar to phase space
expectations. All results are preliminary.Comment: 28 pages, 90 postscript figures, submitted to LP0
Ten simple rules to ruin a collaborative environment
- Author
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- Field of study
A gene expression atlas of the domestic pig
- Author
- A Kauffmann
- A Natividad
- A Quaroni
- A Theocharidis
- A Valbuena
- AB Gyorgy
- AI Su
- AI Su
- Alan L Archibald
- Alasdair Ivens
- Alison Downing
- AM Platt
- Andrew I Su
- Andru Tomoiu
- BA McGivney
- C Thomas
- C Wu
- Christopher K Tuggle
- Chunlei Wu
- CK Tuggle
- CK Tuggle
- CW David
- DA Hume
- DA Hume
- Dario Beraldi
- David A Hume
- David Dorward
- DE Befroy
- E Birney
- F Wu
- G Orwell
- H Lohi
- J Bartek
- J Gorodkin
- J Kenneth Baillie
- J Khattra
- J Soyer
- J Zhang
- JA Rosenfeld
- JE Lattin
- JK Lunney
- JM Vaquerizas
- K Magnusson
- Kim M Summers
- KM Summers
- L Fairbairn
- Lynsey Fairbairn
- M Ashburner
- M Krupp
- M Lukk
- M Uhlen
- M Uhlen
- Mark W Barnett
- MP Terns
- NA Mabbott
- NA Mabbott
- O Britanova
- P Carninci
- P Carninci
- R Kapetanovic
- R Moll
- R Wernersson
- RA Irizarry
- Ramiro Alberio
- RE Thurman
- RJ Wall
- Ronan Kapetanovic
- RS Martherus
- S Brohee
- S van Dongen
- SB Smith
- SC Fahrenkrug
- Sobia Raza
- TC Freeman
- TC Freeman
- TC Freeman
- TMJ Fruchterman
- Tom C Freeman
- TS Heng
- U Ala
- V Vanhorenbeeck
- VR Gordeuk
- W Tang
- X Ge
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
<p>Abstract</p> <p>Background</p> <p>This work describes the first genome-wide analysis of the transcriptional landscape of the pig. A new porcine Affymetrix expression array was designed in order to provide comprehensive coverage of the known pig transcriptome. The new array was used to generate a genome-wide expression atlas of pig tissues derived from 62 tissue/cell types. These data were subjected to network correlation analysis and clustering.</p> <p>Results</p> <p>The analysis presented here provides a detailed functional clustering of the pig transcriptome where transcripts are grouped according to their expression pattern, so one can infer the function of an uncharacterized gene from the company it keeps and the locations in which it is expressed. We describe the overall transcriptional signatures present in the tissue atlas, where possible assigning those signatures to specific cell populations or pathways. In particular, we discuss the expression signatures associated with the gastrointestinal tract, an organ that was sampled at 15 sites along its length and whose biology in the pig is similar to human. We identify sets of genes that define specialized cellular compartments and region-specific digestive functions. Finally, we performed a network analysis of the transcription factors expressed in the gastrointestinal tract and demonstrate how they sub-divide into functional groups that may control cellular gastrointestinal development.</p> <p>Conclusions</p> <p>As an important livestock animal with a physiology that is more similar than mouse to man, we provide a major new resource for understanding gene expression with respect to the known physiology of mammalian tissues and cells. The data and analyses are available on the websites <url>http://biogps.org and http://www.macrophages.com/pig-atlas</url>.</p
Gene Regulation of Intestinal Porcine Epithelial Cells IPEC-J2 Is Dependent on the Site of Deoxynivalenol Toxicological Action
- Author
- AK Diesing
- AK Diesing
- AM Cuervo
- Andreas Post
- Anne-Kathrin Diesing
- BH Liu
- CK Tuggle
- Constanze Nossol
- E Owusu-Ansah
- EL Eskelinen
- G Dennis Jr
- G Koch
- GH Yang
- H Coe
- H Iwahashi
- H Yang
- Hermann-Josef Rothkötter
- Jeannette Kluess
- JH Kouadio
- JM Rhoads
- K Kawai
- KG Steube
- Klaus Wimmers
- M Kitamura
- M Königs
- M Li
- Michael Butterworth
- MW Pfaffl
- Nicole Walk
- P Schierack
- S Dänicke
- S Tsai
- Siriluck Ponsuksili
- SP Cole
- Stefan Kahlert
- T Sergent
- V Mariani
- V Vandenbroucke
- VI Shifrin
- Y Shi
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
The intestinal epithelial cell layer represents the border between the luminal and systemic side of the gut. The decision between absorption and exclusion of substances is the quintessential function of the gut and varies along the gut axis. Consequently, potentially toxic substances may reach the basolateral domain of the epithelial cell layer via blood stream. The mycotoxin deoxynivalenol (DON) is a Fusarium derived secondary metabolite known to enter the blood stream and displaying a striking toxicity on the basolateral side of polarised epithelial cell layers in vitro. Here we analysed potential mechanisms of apical and basolateral DON toxicity reflected in the gene expression. We used the jejunum-derived, polarised intestinal porcine epithelial cell line IPEC-J2 as an in vitro cell culture model. Luminal and systemic DON challenge of the epithelial cell layer was mimicked by a DON application from the apical or basolateral compartment of membrane inserts for 72 h. We compared the genome-wide gene expression of untreated and DON-treated IPEC-J2 cells with the GeneChip® Porcine Genome Array of Affymetrix. Low basolateral DON (200 ng/mL) application triggered 10 times more gene transcripts in comparison to the corresponding apical application (2539 versus 267) despite the intactness of the challenged cell layer as measured by transepithelial electrical resistance. Analysis of the regulated genes by bioinformatic resource DAVID identified several groups of biochemical pathways modulated by concentration and orientation of DON application. Selected genes representing pathways of the cellular metabolism, information processing and structural design were analysed in detail by quantitative PCR. Our findings clearly show that apical and basolateral challenge of epithelial cell layers trigger different gene response profiles paralleled with a higher susceptibility towards basolateral challenge. The evaluation of toxicological potentials of mycotoxins should take this difference in gene regulation dependent on route of application into account
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- 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
- 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
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- 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
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- 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
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- 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 F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck GA
- Beck HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertin A
- Bertinelli F
- Bertolucci F
- Besana MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazek T
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VB
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeriu OEV
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Bracinik J
- Braem A
- Branchini P
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brown H
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- BScher V
- Buanes T
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- 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
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- Zieminska D
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- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
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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
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
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aesky S
- Agar-Savedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- 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 BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- 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
- Andrieux M-L
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
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- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Atkinson M
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen A
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barber T
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- Barnett RM
- Barojas CAC
- Baroncelli A
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- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
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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
Evidence for the h_b(1P) meson in the decay Upsilon(3S) --> pi0 h_b(1P)
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- Zanetti A.
- Zeng Y
- Zeng Y.
- Zeng Y.
- Ziegler V.
- Zucchelli S.
- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Using a sample of 122 million Upsilon(3S) events recorded with the BaBar
detector at the PEP-II asymmetric-energy e+e- collider at SLAC, we search for
the hb(1P) spin-singlet partner of the P-wave chi_{bJ}(1P) states in the
sequential decay Upsilon(3S) --> pi0 h_b(1P), h_b(1P) --> gamma eta_b(1S). We
observe an excess of events above background in the distribution of the recoil
mass against the pi0 at mass 9902 +/- 4(stat.) +/- 2(syst.) MeV/c^2. The width
of the observed signal is consistent with experimental resolution, and its
significance is 3.1sigma, including systematic uncertainties. We obtain the
value (4.3 +/- 1.1(stat.) +/- 0.9(syst.)) x 10^{-4} for the product branching
fraction BF(Upsilon(3S)-->pi0 h_b) x BF(h_b-->gamma eta_b).Comment: 8 pages, 4 postscript figures, submitted to Phys. Rev. D (Rapid
Communications
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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- Abajyan T
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- Abdallah J
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- Zhemchugov A
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- 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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- Winkelmann S
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- Wooden G
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- Xella S
- Xiao M
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- Yabsley B
- Yacoob S
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- 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
- Yu DR
- Yu J
- Yu J
- 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
- Zhang H
- Zhang J
- 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
- 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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