331 research outputs found
Role of the infectious disease consultant in improving antimicrobial therapy prescription in neurosurgery
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
Voxel-wise quantification of myocardial blood flow with cardiovascular magnetic resonance: effect of variations in methodology and validation with positron emission tomography
- Author
- Anita Banerji
- AR Patel
- Christine Tonge
- Christopher A Miller
- Christopher D Steadman
- David Clark
- Deborah Tout
- F Calamante
- F Cecchi
- G Morton
- Geoffrey JM Parker
- Gerry P McCann
- J Biglands
- JM Bland
- JM Bland
- JO Prior
- Josephine H Naish
- JP Greenwood
- JP Parkka
- KL Zierler
- L Axel
- L Ostergaard
- LY Hsu
- M Jerosch-Herold
- M Jerosch-Herold
- M Lortie
- Mark P Ainslie
- Matthias Schmitt
- MM Hajjiri
- N Zarinabad
- NA Pack
- Parthiban Arumugam
- PC Hansen
- PC Hansen
- Peter Weale
- R Wirestam
- RA Dekemp
- Robin M Egdell
- S Laurent
- SA Kajander
- SD Fihn
- SE Petersen
- Simon G Ray
- T Fritz-Hansen
- TF Christian
- TF Christian
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Clustered Gene Expression Changes Flank Targeted Gene Loci in Knockout Mice
- Author
- Abraham Sonenshein
- AE West
- AJ Pocklington
- B Milner
- C Cecchi
- C Li
- C McEwan
- CC Witt
- CM Alberini
- DF Woods
- DJ Linden
- DP Wolfer
- DW Threadgill
- EM Garry
- EM Simpson
- H Bading
- H Husi
- H Husi
- H Husi
- H Tsuda
- JC Tu
- K Hanada
- LC Schalkwyk
- LJ Niedernhofer
- Luis M. Valor
- M Fagiolini
- M Hooper
- M Migaud
- M Tymms
- MO Collins
- MR Kuehn
- NH Komiyama
- P Opazo
- PC Cuthbert
- PV Nguyen
- R Behr
- RC Moore
- S Naisbitt
- S Selbert
- S Yang
- Seth G. N. Grant
- WD Yao
- WE Crusio
- Z Qian
- Publication venue
- Public Library of Science
- Publication date
- 01/12/2007
- Field of study
Gene expression profiling using microarrays is a powerful technology widely used to study regulatory networks. Profiling of mRNA levels in mutant organisms has the potential to identify genes regulated by the mutated protein.Using tissues from multiple lines of knockout mice we have examined genome-wide changes in gene expression. We report that a significant proportion of changed genes were found near the targeted gene.The apparent clustering of these genes was explained by the presence of flanking DNA from the parental ES cell. We provide recommendations for the analysis and reporting of microarray data from knockout mice
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
A new system for quantitative evaluation of infant gaze capabilities in a wide visual field
- Author
- A Guzzetta
- A Macfarlane
- A Madan
- A Morante
- Andrea Pratesi
- C Turati
- Cecilia Laschi
- D Amso
- D Corbetta
- Elena Beani
- F Farzin
- F Farzin
- Francesca Cecchi
- G Gredebäck
- G Gredebäck
- G Sgandurra
- Giovanni Cioni
- Giuseppina Sgandurra
- Hofsten C Von
- J Atkinson
- J Richmond
- JM Leppänen
- LM Dubowitz
- LM Oakes
- M Kato
- M Matsuzawa
- MC Frank
- NZ Kirkham
- OM Blaga
- PA Neil
- Paolo Dario
- PC Quinn
- SP Johnson
- SP Johnson
- SP Johnson
- SP Johnson
- SV Wass
- T Falck-Ytter
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Dor lombar crônica e dor nos membros inferiores em idosas: etiologia em revisão
- Author
- Astin M
- Baumgartner H.
- Borenstein D.
- Burton RR.
- Cecchi F
- Cecchi F
- Creighton D
- Dellaroza MS
- Edmond SL
- Ettinger B
- Eubanks JD
- Eubanks JD
- Fraiman AP.
- Guedes JM
- Hartvigsen J
- Henschke N
- Jones G
- Krieg MA
- Lazaro L 4th
- Leveille SG
- Leveille SG
- Leveille SG
- Leveille SG
- Manchikanti L
- Manchikanti L
- Mazanec DJ.
- Mello TMT
- Melton LJ 3rd
- Musgrave DS
- Nevitt MC
- Pahor M
- Ponka D
- Rudy TE
- Vogt MT
- Vogt MT
- Wing PC.
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Performance studies of the CMS strip tracker before installation
- Author
- Abbaneo D
- Abbas M
- Adam W
- Adler V
- Affolder K
- Affolder T
- Ageron M
- Agram JL
- Ahmed I
- Akhtar I
- Alagoz E
- Albergo S
- Albert E
- Allen A
- Ambroglini F
- Amsler C
- Anagnostou G
- Anghel IM
- Anttila E
- Avanzini C
- Azzi P
- Azzurri P
- Babucci E
- Bacchetta N
- Bagby L
- Bagliesi G
- Bainbridge R
- Balestri G
- Barge D
- Baringer P
- Basti A
- Baulieu G
- Bazterra VE
- Bean A
- Beaumont W
- Beissel F
- Benedetti D
- Benotto F
- Benucci L
- Bergauer T
- Bernardini J
- Berretta L
- Berst JD
- Betchart B
- Bhat PC
- Bianucci S
- Biasini M
- Bilei GM
- Bisello D
- Blaes R
- Bloch C
- Blum P
- Boccali T
- Bocci A
- Bock E
- Bonnet JL
- Bonnevaux A
- Borgia MA
- Borrello L
- Bosi F
- Boudoul G
- Bouhali O
- Bracci F
- Brauer R
- Breuker H
- Brianzi M
- Broccolo B
- Brom JM
- Bruno G
- Buchmuller O
- Buhmann P
- Burke S
- Burkett K
- Butt S
- Butz E
- Callahan D
- Calzolari F
- Campagnari C
- Candelori A
- Caponeri B
- Cardaci M
- Cariola P
- Castaldi R
- Castello R
- Cattai A
- Cazzola U
- Ceccanti M
- Cecchi R
- Cerati GB
- Cerri C
- Chabanat E
- Chabert EC
- Charaf O
- Checcucci B
- Chen J
- Chierici R
- Chiochia V
- Chiorboli M
- Christofek L
- Church I
- Cihangir S
- Ciulli V
- Civinini C
- Clerbaux B
- CMS Collaboration
- Cole JE
- Contardo D
- Costa M
- Costa S
- Coughlan JA
- Covarelli R
- Creanza D
- Cripps N
- Crook A
- Cucoanes AS
- Czellar S
- D'Alessandro R
- D'Alfonso M
- D'Hondt J
- Daubie E
- De Boer W
- De Callatay B
- De Filippis N
- de Langhe E
- De Lentdecker G
- De Mattia M
- De Palma M
- De Robertis G
- De Weirdt S
- De Wolf EA
- Delaere C
- Delattre M
- Dell'Orso R
- Della Negra R
- Delmeire E
- Demaria N
- Demina R
- Devroede O
- Dewulf JP
- Didierjean F
- Dierlamm A
- Dietch J
- Dirkes G
- Dobur D
- Donckt MV
- Dorigo T
- Dragicevic M
- Drouhin F
- Dumitrache F
- Dupasquier T
- Dutta S
- Edera LM
- Elgammal S
- Engstrom P
- Engstrom P
- Eppard M
- Ernenwein JP
- Esser H
- Estre N
- Everaerts P
- Fahrer M
- Fano L
- Farano R
- Feld L
- Ferorelli R
- Fiore L
- Fiori F
- Florins B
- Flucke G
- Flugge G
- Foa L
- Focardi E
- Fontaine JC
- Frey M
- Friedl M
- Frosali S
- Fruhwirth R
- Fulcher J
- Furgeri A
- Galanti M
- Garberson J
- Gateau M
- Gay APR
- Gelin G
- Gennai S
- Genta C
- Gerber CE
- Giammanco A
- Giassi A
- Gill K
- Gillissen C
- Giolo-Nicollerat AS
- Giordano D
- Giorgi MA
- Giraud N
- Giubilato P
- Giudice N
- Giusti S
- Goerlach U
- Goitom I
- Goorens R
- Gotra Y
- Grabit R
- Graehling P
- Gregoire G
- Gritsan AV
- Gross L
- Guardone N
- Guillot G
- Gutsche O
- Hahn KA
- Hale D
- Hall G
- Hamdorf R
- Hammad GH
- Hansel S
- Hanson G
- Harkonen J
- Haroutunian R
- Harris P
- Hartmann F
- Hashemi M
- Hauk J
- Heier S
- Hermanns T
- Heydhausen D
- Heyninck J
- Hinchey C
- Hobson PR
- Hoffmann KH
- Honma A
- Hooper R
- Hosselet J
- Hrubec J
- Huhtinen M
- Incandela H
- Incandela J
- Jaditz S
- Jahn D
- Jeng GY
- Jensen H
- Johnson M
- Juillot P
- Kalavase P
- Kaminski J
- Kaminskiy A
- Karaevski S
- Karimaki V
- Karpinski W
- Kartashov D
- Kaussen G
- Kcira D
- Keutgen T
- Khalatian S
- Khomenkov V
- Klanner R
- Klein K
- Kloukinas K
- Korjenevski S
- Kortesmaa J
- Kostesmaa J
- Kottelat LJ
- Kraan A
- Krammer M
- Kreyer S
- Kukulies C
- Kuronen A
- Kuronen A
- Kyre S
- Lae CK
- Lamb J
- Lampen T
- Landi G
- Landsberg G
- Lariccia P
- Ledermann B
- Lemaitre V
- Lenzi P
- Leonardo N
- Liamsuwan T
- Ligabue F
- Linari S
- Linden T
- Linn A
- Liu H
- Ljuslin C
- Lomtadze T
- Loreti M
- Lounis A
- Lowette S
- Lumb N
- Lungu GA
- Luukka PR
- Luzhetskiy N
- Maazouzi C
- Macchiolo A
- Maenpaa T
- Maes J
- Magazzu G
- Maggi G
- Magini N
- Maletta F
- Mammini P
- Mangano B
- Manna N
- Mannelli M
- Manolescu F
- Mantovani G
- Marage P
- Marcantonini M
- Marchioro A
- Mariani F
- Martin C
- Martinelli G
- Masetti L
- Mason D
- Massa M
- Mattiazzo S
- Mc Guinness C
- Mersi S
- Meschini M
- Messineo A
- Miao T
- Michal S
- Michal S
- Michotte D
- Migliore E
- Militaru O
- Mills C
- Miner D
- Mirabito L
- Moccia S
- Moggi A
- Moulik T
- Mozer M
- Muffat-Joly J
- Muller S
- Muller T
- My S
- Nahn S
- Narain M
- Nguyen D
- Nguyen H
- Nigro M
- Nikolic M
- Noeding C
- Noto F
- Noy M
- Oberegger M
- Olivetto C
- Olzem J
- Onnela A
- Orbaker D
- Ostapchuk A
- Paccagnella A
- Paillard C
- Pal I
- Palla F
- Palmonari F
- Pandoulas D
- Pantano D
- Paoletti S
- Parrini G
- Pasztor G
- Pein U
- Perchalla L
- Pernicka M
- Pernot JF
- Perries S
- Pesaresi M
- Petagna P
- Petit P
- Petragnani G
- Petrucciani G
- Piccut C
- Pierschel G
- Pioppi M
- Piotrzkowski K
- Poettgens M
- Pooth O
- Postema H
- Postolache V
- Potenza R
- Pozzobon N
- Preda M
- Profeti A
- Quertermont L
- Radicci V
- Raffaelli F
- Ranieri R
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- Regenfus C
- Reid ID
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- Vasey F
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- Yumiceva F
- Zaccarelli L
- Zatserklyaniy A
- Zerev E
- Zhukov V
- Zito G
- Zoeller MH
- Zorba O
- Publication venue
- Publication date
- 18/03/2008
- Field of study
Peer reviewe
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta G
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexakhin V
- Alexander J
- Alhusseini M
- Ali MAB Md
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JD Ruiz
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
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- Amsler C
- Anagnostou G
- Anampa K Hurtado
- Anderson D
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- Andreev V
- Andreev Yu
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- Angioni GL Pinna
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- Autermann C
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- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuolo D
- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
- Albert A
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- Alcaraz Maestre J
- Aleksandrov A
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- Allen B
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- Alvarez Fernandez A
- Alvarez JD Ruiz
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
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- Akgun B
- Al-bataineh A
- Albajar C
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- Alcaraz Maestre J
- Aleksandrov A
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- Ali MABM
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
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- Publication venue
- 'Elsevier BV'
- Publication date
- 10/09/2019
- Field of study
The production cross sections of B_{s}^{0} mesons and charge conjugates are measured in proton-proton (pp) and PbPb collisions via the exclusive decay channel B_{s}^{0}→J/ψϕ→μ^{+}μ^{−}K^{+}K^{−} at a center-of-mass energy of 5.02 TeV per nucleon pair and within the rapidity range |y|<2.4 using the CMS detector at the LHC. The pp measurement is performed as a function of transverse momentum (p_{T}) of the B_{s}^{0} mesons in the range of 7 to 50 GeV/c and is compared to the predictions of perturbative QCD calculations. The B_{s}^{0} production yield in PbPb collisions is measured in two p_{T} intervals, 7 to 15 and 15 to 50 GeV/c, and compared to the yield in pp collisions in the same kinematic region. The nuclear modification factor (R_{AA}) is found to be 1.5±0.6(stat)±0.5(syst) for 7–15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15–50 GeV/c, respectively. Within current uncertainties, the B_{s}^{0} results are consistent with models of strangeness enhancement, and suppression by parton energy loss, as observed for the B+ mesons
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