1,019 research outputs found
A Novel Assay to Trace Proliferation History In Vivo Reveals that Enhanced Divisional Kinetics Accompany Loss of Hematopoietic Stem Cell Self-Renewal
- Author
- A Wilson
- AB Lyons
- Anja-Katrin Bielinsky
- CJ Pronk
- D Bryder
- D Bryder
- David Bryder
- E Heilmann
- E Passegue
- EC Forsberg
- F Yan
- G Hoffmann-Fezer
- G Seitz
- GB Bradford
- J Domen
- JA Christian
- Jens M. Nygren
- JM Nygren
- JP Miller
- K Sudo
- M Kondo
- M Osawa
- MB Bowie
- MJ Barnden
- MJ Kiel
- MJ Kiel
- N Yanai
- R Pawliuk
- RV Gardner
- SH Cheshier
- SJ Morrison
- WH Fleming
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
BACKGROUND: The maintenance of lifelong blood cell production ultimately rests on rare hematopoietic stem cells (HSCs) that reside in the bone marrow microenvironment. HSCs are traditionally viewed as mitotically quiescent relative to their committed progeny. However, traditional techniques for assessing proliferation activity in vivo, such as measurement of BrdU uptake, are incompatible with preservation of cellular viability. Previous studies of HSC proliferation kinetics in vivo have therefore precluded direct functional evaluation of multi-potency and self-renewal, the hallmark properties of HSCs. METHODOLOGY/PRINCIPAL FINDINGS: We developed a non-invasive labeling technique that allowed us to identify and isolate candidate HSCs and early hematopoietic progenitor cells based on their differential in vivo proliferation kinetics. Such cells were functionally evaluated for their abilities to multi-lineage reconstitute myeloablated hosts. CONCLUSIONS: Although at least a few HSC divisions per se did not influence HSC function, enhanced kinetics of divisional activity in steady state preceded the phenotypic changes that accompanied loss of HSC self-renewal. Therefore, mitotic quiescence of HSCs, relative to their committed progeny, is key to maintain the unique functional and molecular properties of HSCs
Double hadron leptoproduction in the nuclear medium
- Author
- Airapetian A
- Akopov N
- Akopov Z
- Amarian M
- Andrus A
- Aschenauer EC
- Augustyniak W
- Avakian R
- Avetissian A
- Avetissian E
- Bailey P
- Belostotski S
- Bianchi N
- Blok HP
- Borissov A
- Borysenko A
- Bottcher H
- Brull A
- Bryzgalov V
- Capiluppi M
- Capitani GP
- Ciullo G
- Contalbrigo M
- Dalpiaz PF
- De Leo R
- De Nardo L
- De Sanctis E
- Deconinck W
- Demey M
- Devitsin E
- Di Nezza P
- Diefenthaler M
- Dreschler J
- Duren M
- Ehrenfried M
- Elalaoui-Moulay A
- Elbakian G
- Ellinghaus F
- Elschenbroich U
- Fabbri R
- Fantoni A
- Felawka L
- Frullani S
- Funel A
- Gapienko G
- Gapienko V
- Garibaldi F
- Garrow K
- Gavrilov G
- Gharibyan V
- Giordano F
- Grebeniouk O
- Gregor IM
- Griffioen K
- Guler H
- Hadjidakis C
- Hartig M
- Hasch D
- Hasegawa T
- Hesselink WH
- Hillenbrand A
- Hoek M
- Holler Y
- Hommez B
- Hristova I
- Iarygin G
- Ivanilov A
- Izotov A
- Jackson HE
- Jgoun A
- Kaiser R
- Keri T
- Kinney E
- Kisselev A
- Kobayashi T
- Kopytin M
- Korotkov V
- Kozlov V
- Krauss B
- Kravchenko P
- Krivokhijine VG
- Lagamba L
- Lapikas L
- Lenisa P
- Liebing P
- Linden-Levy LA
- Lorenzon W
- Lu J
- Lu S
- Ma BQ
- Maiheu B
- Makins NCR
- Mao Y
- Marianski B
- Marukyan H
- Masoli F
- Mexner V
- Meyners N
- Michler T
- Mikloukho O
- Miller CA
- Miyachi Y
- Muccifora V
- Murray M
- Nagaitsev A
- Nappi E
- Naryshkin Y
- Negodaev M
- Nowak WD
- Ohsuga H
- Osborne A
- Perez-Benito R
- Pickert N
- Raithel M
- Reggiani D
- Reimer PE
- Reischl A
- Riedl C
- Rith K
- Roelon AR
- Rosner G
- Rostomyan A
- Rubacek L
- Rubin J
- Ryckbosch D
- Salomatin Y
- Sanjiev I
- Savin I
- Schafer A
- Schnell G
- Schuler KP
- Seele J
- Seidl R
- Seitz B
- Shearer C
- Shibata TA
- Shutov V
- Sinram K
- Stancari M
- Statera M
- Steffens E
- Steijger JJM
- Stenzel H
- Stewart J
- Stinzing F
- Streit J
- Tait P
- Tanaka H
- Taroian S
- Tchuiko B
- Terkulov A
- Trzcinski A
- Tytgat M
- van der Nat PB
- van der Steenhoven G
- van Haarlem Y
- Vandenbroucke A
- Veretennikov D
- Vikhrov V
- Vogel C
- Wang S
- Ye Y
- Ye Z
- Yen S
- Zihlmann B
- Zupranski P
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 22/12/2005
- Field of study
First measurement of double-hadron production in deep-inelastic scattering
has been measured with the HERMES spectrometer at HERA using a 27.6 GeV
positron beam with deuterium, nitrogen, krypton and xenon targets. The
influence of the nuclear medium on the ratio of double-hadron to single-hadron
yields has been investigated. Nuclear effects are clearly observed but with
substantially smaller magnitude and reduced A-dependence compared to
previously measured single-hadron multiplicity ratios. The data are in fair
agreement with models based on partonic or pre-hadronic energy loss, while they
seem to rule out a pure absorptive treatment of the final state interactions.
Thus, the double-hadron ratio provides an additional tool for studying
modifications of hadronization in nuclear matter
Treatment of poorly differentiated neuroendocrine tumours with etoposide and cisplatin
- Author
- Publication venue
- Nature Publishing Group
- Publication date
- Field of study
The purpose of this study was to evaluate by a retrospective analysis of 53 patients the efficacy of chemotherapy combining etoposide and cisplatin in the treatment of neuroendocrine tumours. The regimen was a combination of etoposide 100 mg mâ2 dayâ1 for 3 days and cisplatin 100 mg mâ2 on day 1, given by 2-h intravenous infusion, administered every 21 days. Twelve patients had a well-differentiated and 41 a poorly differentiated neuroendocrine tumour. Toxicity of treatment was assessed in 50 patients and efficacy in 52 patients. Among the 11 patients with a well-differentiated tumour evaluable for tumoural response, only one (9.4%) had a partial response for 8.5 months. Forty-one patients with a poorly differentiated tumour showed an objective response rate of 41.5% (four complete and 13 partial responses); the median duration of response was 9.2 months, the median overall survival 15 months and the median progression-free survival 8.9 months. Haematological grade 3â4 toxicity was observed in 60% of the cases with one treatment-related death, digestive grade 3â4 toxicity in 40% and grade 3 alopecia was constant. No severe renal, hearing and neurological toxicities were observed (grade 1 in 6%, 14%, 72% respectively and no grade >1). We confirm that poorly differentiated neuroendocrine tumours are chemosensitive to the etoposide plus cisplatin combination. However, the prognosis remains poor with a 2-year survival lower than 20% confirming that new therapeutic strategies have to be developed. Š 1999 Cancer Research Campaig
Measurement of D-s(+) and D-s(*+) production in B meson decays and from continuum e(+)e(-) annihilation at âs=10.6 GeV
- Author
- Abe K
- Abrams GS
- Adam I
- Adye T
- Albert J
- Aleksan R
- Allison J
- Alsmiller JRG
- Andress JC
- Angelini C
- Anjomshoaa A
- Anthony PL
- Anulli F
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- Azzopardi DE
- BABAR Collaboration
- Back JJ
- Bagnasco S
- Baird K
- Baldini-Ferroli R
- Band HR
- Barillari T
- Barlow NR
- Barlow RJ
- Bartoldus R
- Batignani G
- Bauer JM
- Benayoun M
- Berger N
- Beringer J
- Bernard D
- Bernet R
- Best D
- Bettarini S
- Bhimji W
- Bianchi F
- Bionta RM
- Blaylock G
- Blinov VE
- Bloom E
- 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
- Bright-Thomas PG
- Brigljevic V
- Brochard F
- Brose J
- Brown CM
- Brown D
- Brown DN
- Buchanan C
- Bugg W
- Bukin AD
- Bukin DA
- Bulos F
- Burchat PR
- Button-Shafer J
- Buzykaev AR
- Buzzo A
- Cahn RN
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Carroll 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 AR
- Clark PJ
- Cochran J
- Cohen-Tanugi J
- Cohn H
- Colberg T
- Colecchia F
- Contri R
- Convery MR
- Copty N
- Cottingham WN
- Coupal DP
- Cowan G
- Cowan R
- Coward DH
- Crawley HB
- Cremaldi L
- Crosetti G
- Dahmes B
- Dal Corso F
- Dallapiccola C
- Dasu S
- Dauncey PD
- David P
- Davis CL
- De Groot N
- de la Vaissiere C
- de Lesquen A
- de Monchenault GH
- De Nardo G
- de Sangro R
- Del Buono L
- del Re D
- Della Ricca G
- Deppermann T
- Devmal S
- Di Lodovico F
- Dickopp M
- Dima MO
- Dittongo S
- Dixon P
- Dorfan DE
- Dorfan J
- Dorigo A
- Dubitzky RS
- Dubois-Felsmann GP
- Dunwoodie W
- Dvoretskii A
- Dyce N
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
- Emery S
- Eschenburg V
- Eschrich I
- Fabozzi F
- Faccini R
- Fahey S
- 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
- Fullwood J
- Gabathuler E
- Gabriel TA
- Gaidot A
- Gaillard JM
- Galeazzi F
- Gamba D
- Gamet R
- Ganzhur SF
- Gatto C
- Geddes NI
- Geld TL
- George M
- George S
- Gill MS
- Giorgi MA
- Giraud PF
- Gladney L
- Glanzman T
- Godfrey GL
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy S
- Green MG
- Grillo AA
- Gritsan AV
- Grosdidier G
- Grosso P
- Grothe M
- Groysman Y
- Gunawardane NJW
- Guo QH
- Haas T
- Haire M
- Hamilton R
- Hamon O
- Handler T
- Harrison PF
- Harrison TJ
- Hart PA
- Harton JL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Henderson R
- Hertzbach SS
- Heusch CA
- Hicheur A
- Himel T
- Hitlin DG
- Hocker A
- Hryn'ova T
- Hu H
- Huffer ME
- Innes WR
- Ivanchenko VN
- Iwasaki M
- Izen JM
- Jackson F
- Jackson PD
- Jacobsen RG
- Jawahery A
- Jayatilleke S
- Jessop C
- Johnson DR
- Johnson JR
- Johnson RP
- Jolly S
- Judd D
- Kadel RW
- Kadyk J
- Karyotakis Y
- Kay M
- Kelsey MH
- Kerth LT
- Khan A
- Kim P
- Kirkby D
- Kitayama I
- Knowles DJ
- Koch H
- Kocian ML
- Kofler R
- Kolomensky YG
- Koptchev VG
- Kordich TMB
- Korol AA
- Kowalewski R
- Kozanecki W
- Kral JF
- Kravchenko EA
- Krishnamurthy M
- Kroeger R
- Kunze M
- Kurup A
- Kuznetsova N
- Lacker HM
- Lafferty GD
- Lamanna E
- Lamsa J
- Lanceri L
- Lange D
- Langenegger U
- Langer M
- Lankford AJ
- Laplace S
- Lavin D
- Le Diberder F
- LeClerc C
- Lees JP
- Leith DWGS
- Leonardi E
- Lepeltier V
- Leruste P
- Levi ME
- Levy SL
- Lewandowski B
- Lillard V
- Lista L
- Liu R
- Lo Vetere M
- Lockman WS
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu A
- Lu C
- Luitz S
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Mackay C
- Macri M
- Mallik U
- Maly E
- Mancinelli G
- Mandelkern M
- Manfredi PF
- Margoni M
- Marker CE
- Marsiske H
- Martin JP
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazzoni MA
- McDonald KT
- McGrath P
- McKemey AK
- McKenna JA
- McMahon S
- McMahon TR
- Meadows BT
- Menke S
- Messner R
- Metzler S
- Meyer TI
- Meyer WT
- Michelon G
- Miftakov V
- Milek M
- Moffeit KC
- Monge MR
- Moore TB
- Morandin M
- Morganti M
- Morganti S
- Morii M
- Mount R
- Mugge M
- Muheim F
- Muller DR
- Muller-Pfefferkorn R
- Nash JA
- Nauenberg U
- Neal H
- Neri N
- Nicholson H
- Nief JY
- O'Grady CP
- O'Neale SW
- Ocariz J
- Oddone PJ
- Olivas A
- Olsen J
- Onuchin AP
- Otto S
- Oyang J
- Ozcan VE
- Paick K
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- Palombo F
- Pan Y
- Panetta J
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- Paoloni E
- Paolucci P
- Passaggio S
- Pastore FC
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Penny RC
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petrak S
- Pia MG
- Piccolo D
- Piccolo M
- Piemontese L
- Piredda G
- Plaszczynski S
- Playfer S
- Pompili A
- Poropat P
- Porter FC
- Posocco M
- Potter RJL
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Quinn H
- Rahatlou S
- Rama M
- Rankin P
- Ratcliff BN
- Raven G
- Re V
- Reidy J
- Ricciardi S
- Richman JD
- Rizzo G
- Roat C
- Robbe P
- Roberts DA
- Robertson SH
- Robutti E
- Rochester LS
- Roe NA
- Romosan A
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roussot E
- Roy J
- Ryd A
- Sadrozinski H
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Sanders P
- Sandrelli F
- Santroni A
- Savvas N
- Schaffner SF
- Schalk T
- Schieck JR
- Schietinger T
- Schindler RH
- Schmitz RE
- Schmuecker H
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Sciacca C
- Sciolla G
- Scott I
- Scott IJ
- Seiden A
- Seitz R
- Sekula SJ
- Sen S
- Serbo VV
- Serednyakov SI
- Serfass B
- Serra M
- Sharma V
- Shelkov VG
- Shorthouse HW
- Simi G
- Simonetto F
- Simopoulos ET
- Sinev NB
- Singh H
- Skovpen YI
- Sloane RJ
- Smith AJS
- Smith D
- Smith JG
- Smol A
- Snyder A
- Soffer A
- Soha A
- Sokoloff MD
- Spaan B
- Spanier SM
- Speziali V
- Staengle H
- Stark J
- Steinke M
- Stelzer J
- Stoker DP
- Stroili R
- Strom D
- Strother P
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sutton CS
- Swain JE
- T'Jampens S
- Tanaka HA
- Taras P
- Taylor F
- Tehrani FS
- Telnov AV
- Telnov VI
- Thiebaux C
- Thiessen D
- Tinslay J
- Tisserand V
- Toki WH
- Torassa E
- Tosi S
- Touramanis C
- Treadwell E
- Triggiani G
- Trincaz-Duvoid S
- Tumanov A
- Turnbull L
- Turri M
- Va'vra J
- Vaitsas G
- van Bibber K
- van Hoek WC
- Varnes EW
- Vasileiadis G
- Vasseur G
- Verderi M
- Verkerke W
- Versille S
- Vidal PB
- Voci C
- Voena C
- von Wimmersperg-Toeller JH
- Vuagnin G
- Wagner DL
- Wagner SR
- Wagoner DE
- Waldi R
- Walkowiak W
- Wallom D
- Walsh J
- Wang P
- Watson AT
- Watson NK
- Weatherall JH
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams MI
- Willocq S
- Wilson FF
- Wilson MG
- Wilson RJ
- Wisniewski WJ
- Witherell M
- Wormser G
- Wright DH
- Wright DM
- Wu SL
- Xella SM
- Xie Y
- Yamamoto RK
- Yang S
- Yeche C
- Yellin S
- Young CC
- Yu Z
- Yumiceva FX
- Yushkov AN
- Zacek V
- Zallo A
- Zhang J
- Zhu RY
- Zhu YS
- 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 APSNew measurements of Ds+ and Ds*+ meson production rates from B decays and from qqĚ
continuum events near the ÎĽ(4S) resonance are presented. Using 20.8 fb-1 of data on the ÎĽ(4S) resonance and 2.6 fb-1 off-resonance, we find the inclusive branching fractions B(BâDs+X)=(10.93Âą0.19Âą0.58Âą2.73)% and B(BâDs*+X)=(7.9Âą0.8Âą0.7Âą2.0)%, where the first error is statistical, the second is systematic, and the third is due to the Ds+âĎĎ+ branching fraction uncertainty. The production cross sections Ď(e+e-âDs+X)ĂB(Ds+âĎĎ+)=7.55Âą0.20Âą0.34pb and Ď(e+e-âDs*ÂąX)ĂB(Ds+âĎĎ+)=5.8Âą0.7Âą0.5pb are measured at center-of-mass energies about 40 MeV below the ÎĽ(4S) mass. The branching fractions ÎŁB(BâDs(*)+D(*))=(5.07Âą0.14Âą0.30Âą1.27)% and ÎŁB(BâDs*+D(*))=(4.1Âą0.2Âą0.4Âą1.0)% are determined from the Ds(*)+ momentum spectra. The mass difference m(Ds+)-m(D+)=98.4Âą0.1Âą0.3MeV/c2 is also measured.This work was 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 Swiss NSF, A. P. Sloan Foundation, Research Corporation, and Alexander von Humboldt Foundation
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Beernaert K
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boimska B
- Boldizsar L
- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondu O
- Bontenackels M
- Boos E
- Bornheim A
- Borras K
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- Zumerle G
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
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- Acosta MV
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- Yilmaz Y
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- Yumiceva F
- Yun JC
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- Zakaria M
- Zalewski P
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acosta JG
- Acosta MV
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- Adiguzel A
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- Afanasiev S
- Agostino L
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- Christiansen T
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- Ciulli V
- Civinini C
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- Clerbaux B
- Cline D
- CMS Collaboration
- Coarasa Perez JA
- Cockerill DJA
- Codispoti G
- Colafranceschi S
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- Cooper SI
- Cornelis T
- Correa Martins Junior M
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- Costantini S
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- Coughlan JA
- Cousins R
- Covarelli R
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- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cushman P
- Cussans D
- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Daci N
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- Dahms T
- Dallavalle GM
- Damgov J
- Dammann D
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- Daskalakis G
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- Davies G
- de Barbaro P
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- De La Cruz B
- De La Cruz-Burelo E
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- de Monchenault GH
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
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- Zarubin A
- Zatserklyaniy A
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- Zeyrek M
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
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- Cuevas J
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- Czellar S
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- Da Costa EM
- Dabrowski A
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Abbiendi G
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- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
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- Wrochna G
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- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
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- Yagil A
- Yalvac M
- Yang F
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
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- Yu I
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
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- Zang J
- Zarubin A
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- Zeinali M
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- Zeyrek M
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- Zheng Y
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- Zhukov V
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
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- Afanasiev S
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- Dabrowski A
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- Daubie E
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- de Cassagnac RG
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- De Guio F
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- de Monchenault GH
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
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