726 research outputs found
Study of the reaction e^{+}e^{-} -->J/psi\pi^{+}\pi^{-} via initial-state radiation at BaBar
- Author
- Adametz A
- Adye T
- Ahmed H
- Akar S
- Alam MS
- Albert J
- Andreassen R
- Angelini C
- Anulli F
- Arlen T.
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Aune T.
- Ayad R
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Bard DJ
- Barlow RJ
- Bartoldus R
- Batignani G
- Behera PK
- Behn E
- Beilicke M.
- Bellis M
- Ben-Haim E
- Benbow W.
- Benitez JF
- Bernard D
- Bernlochner FU
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bianchi F
- Biasini M
- Biassoni P
- Blinov VE
- Bloom PC
- Bomben M
- Bondioli M
- Bonneaud GR
- Bouvier A.
- Bozzi C
- Bradbury S. M.
- Brau J
- Briand H
- Brown DN
- Brown DN
- Buckley J. H.
- Bugaev V.
- Bunger C
- Burchat PR
- Buzykaev AR
- Byrum K.
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Cannon A.
- Cara M.
- Carpinelli M
- Cartaro C
- Casadio C.
- Casarosa G
- Cenci R
- Cervelli A
- Cesarini A.
- Chao DS
- Chauveau J
- Chavez CA
- Cheaib R
- Chen C
- Cheng CH
- Cheung C. C.
- Choi HHF
- Cibinetto G
- Ciupik L.
- Clark PJ
- Cochran J
- Coleman JP
- Connolly M. P.
- Contri R
- Convery MR
- Cowan G
- Cowan R
- Cremaldi L
- Cui W.
- Dallapiccola C
- Dasu S
- Dauncey PD
- Davier M
- Davies F.
- Davis CL
- de Almeida U. Barres
- de Monchenault GH
- De Nardo G
- de Sangro R
- Denig AG
- Derkach D
- Di Lodovico F
- Dickherber R.
- Doi A.
- Dorfan J
- Druzhinin VP
- Dubois-Felsmann GP
- Dujmic D
- Duke C.
- Dunwoodie W
- Ebert M
- Echenard B
- Edwards AJ
- Eigen G
- Eisner AM
- Emery S
- Ernst JA
- Errando M.
- Faccini R
- Falcone A.
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finley J. P.
- Finnegan G.
- Finocchiaro G
- Fioravanti E
- Flood KT
- Ford WT
- Forti F
- Fortson L.
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Furniss A.
- Gabareen AM
- Gabathuler E
- Gagliardi N
- Galante N.
- Gall D.
- Gamba D
- Gary JW
- Garzia I
- Gaspero M
- Gaz A
- Gershon TJ
- Gioi LL
- Giorgi MA
- Giovannini G.
- Giroletti M.
- Godambe S.
- Godang R
- Golubev VB
- Gorodeisky R
- Gradl W
- Graham MT
- Grauges E
- Grenier P
- Griessinger K
- Griffin S.
- Gritsan AV
- Grosdidier G
- Grube J.
- Grunberg O
- Guido E
- Guo ZJ
- Guttman N
- Gyuk G.
- Hada K.
- Hafner A
- Hamilton B
- Hamon O
- Hanna D.
- Hardee P.
- Harris D. E.
- Harrison PF
- Hartmann T
- Hast C
- Hearty C
- Hitlin DG
- Holder J.
- Hong TM
- Honscheid K
- Huan H.
- Huard Z
- Hui C. M.
- Hutchcroft DE
- Innes WR
- Izen JM
- Jackson G
- Jawahery A
- Jessop CP
- Junor W.
- Kaaret P.
- Karlsson N.
- Kass R
- Kelsey MH
- Kerth LT
- Kertzman M.
- Khan A
- Khassen Y.
- Kieda D.
- Kim P
- King GJ
- Kino M.
- Kirkby D
- Koch H
- Kocian ML
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kravchenko EA
- Krawczynski H.
- Krennrich F.
- Kroeger R
- Kroseberg J
- Lacker HM
- Lafferty GD
- Lanceri L
- Lang M. J.
- Lange DJ
- Lankford AJ
- Latham TE
- Le Diberder F
- LeBohec S.
- Leddig T
- Lee CL
- Lee N. P.
- Lees JP
- Leith DWGS
- Leruste P
- Lewczuk MJ
- Lewis P
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman WS
- Long O
- LoSecco JM
- Lou XC
- Lueck T
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Ly C.
- Lynch G
- Lynch HL
- MacFarlane DB
- Madrid J.
- Maier G.
- Malaescu B
- Mallik U
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Martinelli M
- Martinez AJ
- Martinez-Vidal F
- Massaro F.
- Mattison TS
- Mazzoni MA
- McArthur S.
- McCann A.
- McConville W.
- McKenna JA
- Meadows BT
- Meyer WT
- Miyashita TS
- Monge MR
- Monorchio D
- Morandin M
- Moriarty P.
- Morii M
- Mukherjee R.
- Muller DR
- Mundell C. G.
- Munerato M
- Nagai H.
- Nauenberg U
- Neal H
- Negrini M
- Nelson S
- Neri N
- Nguyen X
- Nugent IM
- Nunez P. D.
- Oberhof B
- Ocariz J
- Olaiya EO
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- Onorato G
- Onuchin AP
- Orr M.
- Otte A. N.
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- Pacetti S
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- Perez A
- Perkins J. S.
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- Peruzzi IM
- Piccolo M
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- Piemontese L
- Piredda G
- Playfer S
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- Poireau V
- Porter FC
- Posocco M
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- Prokoph H.
- Puccio EMT
- Pulliam T
- Purohit MV
- Ragan K.
- Rakitin AY
- Rama M
- Randle-Conde A
- Ratcliff BN
- Raven G
- Reyes L. C.
- Reynolds P. T.
- Richman JD
- Ritchie JL
- Rizzo G
- Roache E.
- Roberts DA
- Robertson SH
- Robutti E
- Roney JM
- Roodman A
- Rose H. J.
- Rossi A
- Rotondo M
- Roudeau P
- Rubin AE
- Ruland AM
- Ruppel J.
- Sacco R
- Salnikov AA
- Santoro V
- Schindler RH
- Schroder H
- Schroeder T
- Schroedter M.
- Schubert KR
- Schumm BA
- Schune MH
- Schwierz R
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Sembroski G. H.
- Sentuerk G. D.
- Serednyakov SI
- Sevilla MF
- Sigamani M
- Sillanpaa A.
- Simard M
- Simi G
- Simonetto F
- Sinev NB
- Sitarek J.
- Sitt S
- Skovpen YI
- Smith AJS
- Smith JG
- Snyder A
- Sobczynska D.
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Sonnek P
- Spaan B
- Spanier F.
- Spanier SM
- Spiro S.
- Stamerra A.
- Steele I. A.
- Steinke B.
- Stocchi A
- Storz J.
- Stracka S
- Strah N.
- Stroili R
- Strom D
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sun L
- Suric T.
- Takalo L.
- Takami H.
- Taras P
- Tasneem N
- Tavecchio F.
- Telezhinsky I.
- Telnov AV
- Temnikov P.
- Terzic T.
- Tescaro D.
- Teshima M.
- Tesic G.
- Theiling M.
- Thibadeau S.
- Thom M.
- Tibolla O.
- Tico JG
- Tisserand V
- Todyshev KY
- Toki WH
- Torrence E
- Torres D. F.
- Touramanis C
- Treves A.
- Uwer U
- Va'vra J
- Vankov H.
- Varlotta A.
- Vasseur G
- Vassiliev V. V.
- Verderi M
- Vitale L
- Vitug GM
- Vivier M.
- Vogler P.
- Voss C
- Wagner AP
- Wagner R. M.
- Wagner SR
- Wakely S. P.
- Waldi R
- Walker R. C.
- Walsh JJ
- Wang WF
- Weekes T. C.
- Weitzel Q.
- West CA
- White RM
- Williams D. A.
- Wilson FF
- Wilson JR
- Wisniewski WJ
- Wittgen M
- Wood D. L.
- Wormser G
- Wray BC
- Wright DH
- Wright DM
- Wu SLL S. N.
- Wulsin HW
- Yeche C
- Young CC
- Yushkov AN
- Zabalza V.
- Zallo A
- Zandanel F.
- Zanin R.
- Ziegler V
- Zitzer B.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We study the process e+e−→J/ψπ+π− with
initial-state-radiation events produced at the PEP-II asymmetric-energy
collider. The data were recorded with the BaBar detector at center-of-mass
energies 10.58 and 10.54 GeV, and correspond to an integrated luminosity of 454
fb−1. We investigate the J/ψπ+π− mass
distribution in the region from 3.5 to 5.5 GeV/c2. Below 3.7
GeV/c2 the ψ(2S) signal dominates, and above 4
GeV/c2 there is a significant peak due to the Y(4260). A fit to
the data in the range 3.74 -- 5.50 GeV/c2 yields a mass value
4244±5 (stat) ±4 (syst)MeV/c2 and a width value 114−15+16 (stat)±7(syst)MeV for this state. We do not
confirm the report from the Belle collaboration of a broad structure at 4.01
GeV/c2. In addition, we investigate the π+π− system
which results from Y(4260) decay
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
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- 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
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- Alves GA
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- 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
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- Attikis A
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- Autermann C
- Auzinger G
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- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
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- Baesso P
- Baffioni S
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- Bai Y
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- Baumgartel D
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- Bazterra VE
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- Cortezon EP
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- Dauncey P
- David A
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- de Barbaro P
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- Edelmaier CJ
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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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
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- Ziebarth EB
- Ziegler J
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- Zoeller MH
- Zotto P
- Zou W
- 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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- CMS Collaboration
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- Cripps N
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- Cuplov V
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- Cutajar M
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- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
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- Da Costa EM
- Da Silva WLP
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- Eugster J
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- Kaftanov V
- Kailas S
- Kalakhety H
- Kalavase P
- Kalinowski A
- Kalogeropoulos A
- Kamenev A
- Kamon T
- Kang S
- Kangal EE
- Kannike K
- Kao KY
- Kao SC
- Kapusi A
- Karaman T
- Karapostoli G
- Karavakis E
- Karchin PE
- Karim M
- Karimaki V
- Karjavin V
- Karmgard DJ
- Kaschube K
- Kasemann M
- Kasieczka G
- Kataria SK
- Katkov I
- Katsas P
- Kaufman GN
- Kaur M
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- Kaya M
- Kaya O
- Kazana M
- Kcira D
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- Kellogg RG
- Kelly T
- Kennedy BW
- Kesisoglou S
- Khachatryan V
- Khakzad M
- Khalatyan S
- Khalil S
- Khan A
- Khan WA
- Kharchilava A
- Khatiwada R
- Khotilovich V
- Khukhunaishvili A
- Khurshid T
- Kiesenhofer W
- Killewald P
- Kilminster B
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- Kirakosyan M
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- Klanner R
- Klapoetke K
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- Klem J
- Klima B
- Klimenko S
- Klimkovich T
- Klingebiel D
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- Knutsson A
- Ko W
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- Kodolova O
- Kohli JM
- Kokkas P
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- Konecki M
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- Konstantinov D
- Kopecky A
- Korablev A
- Korpela A
- Kortelainen MJ
- Korytov A
- Kossov M
- Kotlinski D
- Kotov K
- Kousouris K
- Kovalskyi D
- Kovitanggoon K
- Koybasi O
- Kozhuharov V
- Kozlov G
- Kraan A
- Krajczar K
- Kramer L
- Krammer M
- Krasnikov N
- Kravchenko I
- Kreczko L
- Kreis B
- Kress M
- Kress T
- Kreuzer P
- Kroeger R
- Krofcheck D
- Krokhotin A
- Krolikowski J
- Kropivnitskaya A
- Krpic D
- Krucker D
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- Krychkine V
- Kubik A
- Kubota Y
- Kuessel Y
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- Kukartsev G
- Kumar A
- Kumar A
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- Kuo CM
- Kurca T
- Kurt R
- Kuznetsov V
- Kuznetsova E
- Kwan S
- Kyberd P
- Kypreos T
- Kyriakis A
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- Lacaprara S
- Lacroix F
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- Laird E
- Lamichhane R
- Lampen T
- Lanaro A
- Lander R
- Landsberg G
- Lanev A
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- Lange W
- Langenegger U
- Lannon K
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- Laszlo A
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- Lazzizzera I
- Le Bihan AC
- Le Grand T
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- Lecomte P
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- Ledovskoy A
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- Lee KS
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- Letts J
- Levchenko P
- Levchuk L
- Li SW
- Li W
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- Liao J
- Ligabue F
- Liko D
- Limon P
- Lin C
- Lin W
- Linares EC
- Linden T
- Ling TY
- Linn A
- Linn S
- Lipton R
- Lista L
- Litov L
- Litvine V
- Liu C
- Liu F
- Liu H
- Liu H
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- Liu MH
- Liu YF
- Liu ZK
- Llatas M
- Locci E
- Lohmann W
- Loizides C
- Lokhtin I
- Lomidze D
- Lomtadze T
- Longo E
- Lopez A
- Lopez EL
- Lopez O
- Lopez S
- Lopez-Fernandez R
- Loukas D
- Lourenco C
- Loveless R
- Lowette S
- Lu RS
- Lu Y
- Lu YJ
- Lucaroni A
- Luckey R
- Lundstedt C
- Lungu G
- Luo W
- Lusito L
- Lustermann W
- Luthra A
- Luukka P
- Lychkovskaya N
- Lykken J
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- Lyons L
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- Ma Y
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- Maenpaa T
- Maes J
- Maes M
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- Maestre JA
- Magass C
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- Maguire C
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- Majumder G
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- Makouski M
- Maksimovic R
- Malberti M
- Malbouisson H
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- Malek M
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- Malik S
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- Mangano B
- Mankel R
- Manna N
- Mannelli M
- Manolakos I
- Mans J
- Manthos N
- Mantovani G
- Mao Y
- Marage PE
- Marangelli B
- Maravin Y
- Marcellini S
- Marchica C
- Marco J
- Marco R
- Margoni M
- Marienfeld M
- Marinelli N
- Marinho F
- Marinov A
- Marinova E
- Marionneau M
- Mariotti C
- Markou A
- Markou C
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- Marlow D
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- Maroussov V
- Marraffino JM
- Marrouche J
- Martelli A
- Martin MA
- Martin W
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- Martini L
- Martins CD
- Martins R
- Martisiute D
- Martschei D
- Maruyama S
- Maselli S
- Masetti G
- Masetti L
- Mason D
- Massironi A
- Matchev K
- Mateev M
- Mathias B
- Matorras F
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- Matveev V
- Mavrommatis C
- Mazumdar K
- Mazzucato M
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- McCauley T
- McCliment E
- Mccoll N
- Medvedeva T
- Megrelidze L
- Mehdiabadi SP
- Mehta MZ
- Meier F
- Meijers F
- Mejias BM
- Mekterovic D
- Melo A
- Melzer-Pellmann IA
- Menasce D
- Mendez H
- Meneghelli M
- Meneguzzo AT
- Menendez JF
- Menichelli M
- Mercier D
- Meridiani P
- Merino G
- Merkel P
- Merlo JP
- Mermerkaya H
- Merola M
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- Mersi S
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- Merz J
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- Mesropian C
- Messineo A
- Mestvirishvili A
- Metson S
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- Meyer AB
- Miao T
- Miceli T
- Migliore E
- Mignerey AC
- Mikami Y
- Mikulec I
- Mila G
- Milenovic P
- Militaru O
- Miller DH
- Millischer L
- Milosevic J
- Milstene C
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- Miner DC
- Mirabito L
- Mironov C
- Mishra K
- Mitselmakher G
- Mnich J
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- Mohammadi A
- Mohanty AK
- Mohanty GB
- Mohapatra A
- Mohr N
- Moisenz P
- Molnar J
- Monaco V
- Mondal NK
- Montalvo R
- Montanari A
- Montanino D
- Montoya CAC
- Moon DH
- Mooney M
- Moortgat F
- Moreno BG
- Moreno S
- Moroni L
- Morovic S
- Morse DM
- Moser R
- Mossolov V
- Mott A
- Mousa J
- Mozer MU
- Mrenna S
- Mucibello L
- Mueller S
- Muelmenstaedt J
- Muentel M
- Mulders M
- Muller T
- Mundim L
- Muniz L
- Mura B
- Murray M
- Murzin V
- Musella P
- Musenich R
- Musich M
- Musienko Y
- Mussgiller A
- My S
- Nachtman J
- Nahn S
- Najafabadi MM
- Nandi R
- Nappi A
- Narain M
- Nart A
- Nash J
- Nauenberg U
- Naumann-Emme S
- Navarria FL
- Nawrocki K
- Nayak A
- Nef P
- Nessi-Tedaldi F
- Nesvoldl E
- Neu C
- Neumeister N
- Newbold DM
- Newman HB
- Newman-Holmes C
- Newsom CR
- Nguyen CN
- Nguyen D
- Nguyen H
- Nguyen M
- Nicolaou C
- Niegel M
- Nikitenko A
- Nikolic M
- Nirunpong K
- Nishu N
- Nogima H
- Noli P
- Noonan D
- Norbeck E
- Nourbakhsh S
- Novaes SF
- Nowack A
- Nowak F
- Ntomari E
- Nuzzo S
- O'Brien C
- O'Dell V
- Oberst O
- Obertino MM
- Obraztsov S
- Ocalan K
- Ochando C
- Ochesanu S
- Odell N
- Odorici F
- Oehler A
- Ofierzynski RA
- Oguri V
- Olaiya E
- Oliveros AFO
- Oliveros S
- Olsen J
- Olson J
- Olzem J
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- Orbaker D
- Oreshkin V
- Organtini G
- Orimoto T
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- Osipenkov I
- Ostapchuk A
- Ott J
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- Ozdemir K
- Ozkorucuklu S
- Ozok F
- Ozpineci A
- Ozturk S
- Pacifico N
- Padhi S
- Padley BP
- Padula SS
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- Pagano D
- Paganoni M
- Pakhotin Y
- Palichik V
- Palinkas J
- Palla F
- Palma A
- Palmer C
- Palmonari F
- Panagiotou A
- Pandolfi F
- Pant LM
- Panwalkar S
- Paoletti S
- Paolucci P
- Papacz P
- Papadopoulos I
- Papageorgiou A
- Pape L
- Paramatti R
- Parashar N
- Pardo P
- Pardos C
- Parenti A
- Park C
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- Parracho PC
- Pashenkov A
- Pastrone N
- Patel R
- Patras V
- Patterson JR
- Paulini M
- Paus C
- Pauss F
- Pavlov B
- Pavlunin V
- Pearson T
- Pedrini D
- Pegna DL
- Peiffer T
- Pelayo J
- Pellett D
- Pelliccioni M
- Penzo A
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- Pereira AV
- Perelygin V
- Perera L
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- Perez JAC
- Perieanu A
- Pernicka M
- Perries S
- Perrotta A
- Perrozzi L
- Pesaresi M
- Petkov P
- Petrakou E
- Petridis K
- Petrilli A
- Petrillo G
- Petrov P
- Petrov V
- Petrucciani G
- Petrushanko S
- Petyt D
- Pfeiffer A
- Pi H
- Piccolo D
- Pieri M
- Pierini M
- Pierro GA
- Pieta H
- Pietsch N
- Pimia M
- Pin A
- Pineda AM
- Pioppi M
- Piotrzkowski K
- Piparo D
- Piperov S
- Piroue R
- Pivarski J
- Plager C
- Plestina R
- Pol ME
- Polatoz A
- Polese G
- Polic D
- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popescu S
- Pordes R
- Pozdnyakov A
- Pozzobon N
- Prescott C
- Primavera F
- Prokofyev O
- Prosper H
- Ptochos F
- Pugliese G
- Puigh D
- Puljak I
- Punz T
- Qazi S
- Qian SJ
- Quan X
- Quast G
- Quertenmont L
- Rabbertz K
- Racz A
- Radburn-Smith BC
- Radicci V
- Ragazzi S
- Rahatlou S
- Rahmat R
- Raics P
- Raidal M
- Rakness G
- Ralich R
- Ralph D
- Ramos FD
- Ramos JP
- Rander J
- Ranieri R
- Rappoccio S
- Raspereza A
- Ratnikov F
- Raupach F
- Raval A
- Raymond DM
- Razis PA
- Rebane L
- Rebassoo E
- Redaelli N
- Redjimi R
- Redondo I
- Reeder D
- Regenfus C
- Reid ID
- Reithler H
- Rekovic V
- Remington R
- Renker D
- Rennefeld J
- Renz M
- Reucroft S
- Reyes-Santos MA
- Rhee HB
- Ribeiro PQ
- Ribnik J
- Riccardi C
- Richards A
- Richman J
- Rikova MI
- Riley D
- Rios AAO
- Rivero C
- Rizzi A
- Roberts J
- Robles J
- Robmann P
- Rodenburg M
- Rodozov M
- Rodrigo T
- Rodriguez JL
- Rogan C
- Roh Y
- Rohe T
- Rohlf J
- Rohringer H
- Roinishvili V
- Roland B
- Roland C
- Roland G
- Rolandi G
- Romano E
- Romanowska-Rybinska K
- Romero A
- Romero L
- Rommerskirchen T
- Rompotis N
- Ronchese P
- Ronga FJ
- Rose A
- Rose K
- Roselli G
- Rosowsky A
- Ross I
- Rossato K
- Rossi AM
- Rossin R
- Rossini M
- Rougny R
- Rovelli C
- Rovelli T
- Rovere M
- Ruchti R
- Rudolph M
- Rumerio P
- Rusack R
- Rusakov SV
- Ruspa M
- Russ J
- Ryan MJ
- Ryckbosch D
- Ryd A
- Rykaczewski H
- Ryu G
- Ryutin R
- Sabes D
- Sabonis T
- Sacchi R
- Safarzadeh B
- Safonov A
- Safronov G
- Saha A
- Saini LK
- Saka H
- Sakharov A
- Sakulin H
- Sala L
- Sala S
- Salerno R
- Salur S
- Sammet J
- Sanabria JC
- Sanchez AK
- Sanchez FJ
- Sanchez J
- Sanchez MCDLB
- Sander C
- Sanders DA
- Sanders S
- Sani M
- Santanastasio F
- Santaolalla J
- Santocchia A
- Santoro A
- Sanudo M
- Saoulidou N
- Saout C
- Sarkar S
- Sarycheva L
- Sasseville M
- Sauerland P
- Savin A
- Savrin V
- Sawley MC
- Schael S
- Schafer C
- Schettler H
- Scheurer A
- Schieferdecker P
- Schilling FP
- Schlein P
- Schleper P
- Schmidt A
- Schmidt R
- Schmitt M
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoerner-Sadenius T
- Schofbeck R
- Schott G
- Schroder M
- Schul N
- Schum T
- Schwandt J
- Schwarz T
- Schwick C
- Scodellaro L
- Scurlock B
- Searle M
- Seez C
- Segala M
- Segneri G
- Segoni I
- Seixas J
- Sekmen S
- Sellers P
- Selvaggi G
- Selvaggi M
- Semenov S
- Sen N
- Sen S
- Sengupta S
- Senkin S
- Seo E
- Seo H
- Serban AT
- Serin M
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- Sguazzoni G
- Sharma A
- Sharma A
- Sharma S
- Sharma V
- Sharp P
- Sheldon P
- Shen BC
- Shepherd-Themistocleous CH
- Shi X
- Shin S
- Shipkowski SP
- Shipsey I
- Shiu JG
- Shivpuri RK
- Shmatov S
- Shrestha S
- Shreyber I
- Shukla P
- Shumeiko N
- Sibille J
- Siegrist P
- Sierra RV
- Sikler F
- Sill A
- Sillou D
- Silva P
- Silvers D
- Silverwood H
- Silvestre C
- Silvestris L
- Sim KS
- Simon M
- Simon S
- Simonetto F
- Simonis HJ
- Singh AP
- Singh JB
- Singh SP
- Singovsky A
- Sirois Y
- Siroli G
- Sirunyan AM
- Skhirtladze N
- Skuja A
- Slabospitsky S
- Slaunwhite J
- Smirnov I
- Smirnov V
- Smith J
- Smith JG
- Smith K
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- Smith WH
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- Sobol A
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- Somalwar S
- Son D
- Son DC
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- Sonmez N
- Sonnenschein L
- Sordini V
- Souza MHG
- Spagnolo P
- Spalding WJ
- Spanier S
- Sparrow A
- Speer T
- Sperka D
- Sphicas P
- Spiegel L
- Spiga D
- Spiropulu M
- Sprenger D
- Squires M
- Srivastava AK
- Stadie H
- Stahl A
- Staiano A
- Starodumov A
- Steggemann J
- Stein M
- Steinbruck G
- Stenson K
- Stephans GSF
- Stickland D
- Stieger B
- Stober FM
- Stockli F
- Stolin V
- Stone R
- Stoye M
- Stoykova S
- Stoynev S
- Strauss J
- Stringer R
- Strom D
- Stuart D
- Sturdy J
- Suarez RG
- Sudhakar K
- Sulak L
- Sulimov V
- Sultanov G
- Summers D
- Sumorok K
- Sumowidagdo S
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- Surat UE
- Svintradze I
- Svyatkovskiy A
- Swain J
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- Swartz M
- Szillasi Z
- Szleper M
- Sznajder A
- Tali B
- Tan R
- Tancini V
- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
- Tauscher L
- Tavernier S
- Taylor L
- Tcholakov V
- Teischinger F
- Temple J
- Tenchini R
- Teng H
- Teo WD
- Teodorescu L
- Terentyev N
- Teyssier D
- Thea A
- Theofilatos K
- Thiebaux C
- Thom J
- Thomas L
- Thomas M
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- Thomsen J
- Thyssen F
- Timciuc V
- Titov M
- Tkaczyk S
- To W
- Toback D
- Tomalin IR
- Tomaszewska J
- Tomei TRFP
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- Tonjes MB
- Tonwar SC
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- Tornier D
- Toropin A
- Torre P
- Tosi M
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- Tourneur S
- Tourtchanovitch L
- Traczyk P
- Tran NV
- Travaglini R
- Trayanov R
- Treille D
- Trentadue R
- Triantis FA
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropea P
- Tropiano A
- Troshin S
- Tsang KV
- Tschudi Y
- Tsirou A
- Tsyganov A
- Tu Y
- Tucker J
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Tupputi S
- Tuuva T
- Tuve C
- Twedt E
- Tytgat M
- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
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- Valdez HC
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- Van Onsem GP
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- Vanelderen L
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- Vankov I
- Vanlaer R
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- Vazquez DD
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- Velasco M
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- Velkovska J
- Venturi A
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- Verdini PG
- Veresil GI
- Vergili LN
- Vergili M
- Verrecchia P
- Verwilligen R
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vichoudis P
- Vidal R
- Vila I
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Virto A
- Vishnevskiy D
- Vitulo P
- Viviani C
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
- Volpe R
- Volyanskyy D
- Vorobiev I
- Vorobyev A
- Voutilainen M
- Wagner P
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Walsh R
- Walsh S
- Waltenberger W
- Walzel G
- Wan Z
- Wang D
- Wang J
- Wang J
- Wang M
- Wang X
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- Warchol J
- Ward S
- Wardrope D
- Wayne M
- Weber H
- Weber M
- Weber M
- Wehrli L
- Weinberg M
- Weinberger M
- Wendland L
- Weng J
- Weng Y
- Wenger EA
- Werner JS
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickens J
- Wickramage N
- Widl E
- Wigmans R
- Wilken R
- Wilkinson R
- Williams G
- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Wohri HK
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu JH
- Wu W
- Wulz CE
- Wurthwein F
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yan M
- Yang F
- Yang M
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
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
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
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- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
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- Aguilar-Benitez M
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- Ahmad WH
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- Wissing C
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- Won S
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- Wood JS
- Worm SD
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- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
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- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zotto P
- Zou W
- 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
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- 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
- Alcaraz Maestre J
- Alda Junior WL
- Aldaya Martin M
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- 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
- Antonelli L
- Antunovic Z
- Apanasevich L
- Appelt E
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Barfuss AF
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- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
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- Bartalini P
- Barth C
- Basegmez S
- Basso L
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- Yilmaz Y
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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
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
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- Alcaraz Maestre J
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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
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Temple J
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- Teo WD
- Teodorescu L
- Teyssier D
- Thea A
- Theofilatos K
- Thom J
- Thomas L
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- Thyssen F
- Tiko A
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- Tran NV
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- Turner M
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- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ulrich R
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- Uplegger L
- Urscheler C
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- Uzunian A
- Vaandering EW
- Valls N
- Valuev V
- Van Doninck W
- Van Haevermaet H
- Van Hove P
- Van Mechelen P
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- Vergili M
- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Vischia P
- Vishnevskiy D
- Vitulo P
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner P
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Walsh R
- Walsh S
- Waltenberger W
- Walzel G
- Wan X
- Wang J
- Wang J
- Wang M
- Wang S
- Wang X
- Wang Z
- Wardle N
- Wasserbaech S
- Wayand S
- Wayne M
- Weber H
- Weber HA
- Weber M
- Weber M
- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
- Weng Y
- Wenger EA
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickramage N
- Widl E
- Wilken R
- Wilkinson R
- Williams G
- Williams T
- Willmott C
- Wimpenny S
- Winer BL
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
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- Wood JS
- Worm SD
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- Wuerthwein F
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- Wyslouch B
- Xiao H
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- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- 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
Orientation of the Calcium Channel β Relative to the α12.2 Subunit Is Critical for Its Regulation of Channel Activity
- Author
- A Castellano
- AC Dolphin
- AC Dolphin
- AE Lacerda
- Aleksandr Shcheglovitov
- Arnold Schwartz
- AT Leung
- C Geourjon
- CJ Frazier
- CL Vance
- D Singer
- D Walker
- E Perez-Reyes
- Edward Perez-Reyes
- F Van Petegem
- G Sandoz
- G Sandoz
- GD Malo
- GJ Stephens
- HL Agler
- I Vitko
- II Arias-Olguín
- Imilla I. Arias-Olguín
- Iuliia Vitko
- J Arikkath
- J Leroy
- J Striessnig
- Janet Murbartián
- JB Harry
- JM Arias
- JM Schjott
- Joel P. Baumgart
- JP Baumgart
- Juan Manuel Arias
- L Birnbaumer
- LL He
- M Pragnell
- M Wakamori
- M Wolf
- MJ Berridge
- MR Hanlon
- MW Richards
- N Qin
- N Qin
- NC Shaner
- NM Soldatov
- PF Brust
- RM Cohen
- S Geib
- S Hering
- S Ringer
- S Sokolov
- SB Long
- SX Takahashi
- T Gonoi
- T Yasuda
- TD Helton
- TK Kerppola
- VE Scott
- Y Mori
- Y Opatowsky
- Y-H Chen
- YJ Shyu
- Z Lin
- Z-P Feng
- Publication venue
- Public Library of Science
- Publication date
- 29/10/2008
- Field of study
BACKGROUND: The Ca(v)beta subunits of high voltage-activated Ca(2+) channels control the trafficking and biophysical properties of the alpha(1) subunit. The Ca(v)beta-alpha(1) interaction site has been mapped by crystallographic studies. Nevertheless, how this interaction leads to channel regulation has not been determined. One hypothesis is that betas regulate channel gating by modulating movements of IS6. A key requirement for this direct-coupling model is that the linker connecting IS6 to the alpha-interaction domain (AID) be a rigid structure. METHODOLOGY/PRINCIPAL FINDINGS: The present study tests this hypothesis by altering the flexibility and orientation of this region in alpha(1)2.2, then testing for Ca(v)beta regulation using whole cell patch clamp electrophysiology. Flexibility was induced by replacement of the middle six amino acids of the IS6-AID linker with glycine (PG6). This mutation abolished beta2a and beta3 subunits ability to shift the voltage dependence of activation and inactivation, and the ability of beta2a to produce non-inactivating currents. Orientation of Ca(v)beta with respect to alpha(1)2.2 was altered by deletion of 1, 2, or 3 amino acids from the IS6-AID linker (Bdel1, Bdel2, Bdel3, respectively). Again, the ability of Ca(v)beta subunits to regulate these biophysical properties were totally abolished in the Bdel1 and Bdel3 mutants. Functional regulation by Ca(v)beta subunits was rescued in the Bdel2 mutant, indicating that this part of the linker forms beta-sheet. The orientation of beta with respect to alpha was confirmed by the bimolecular fluorescence complementation assay. CONCLUSIONS/SIGNIFICANCE: These results show that the orientation of the Ca(v)beta subunit relative to the alpha(1)2.2 subunit is critical, and suggests additional points of contact between these subunits are required for Ca(v)beta to regulate channel activity
The enigmatic mitochondrial genome of Rhabdopleura compacta (Pterobranchia) reveals insights into selection of an efficient tRNA system and supports monophyly of Ambulacraria
- Author
- A Grigoriev
- A Hassanin
- A Kondow
- A Reyes
- A Scouras
- A Scouras
- C Notredame
- CB Cameron
- CJ Winchell
- D Ojala
- Detlef Bernhard
- DV Lavrov
- DW Schultz
- DW Schultz
- F Abascal
- F Abascal
- F Ronquist
- IJ Holt
- IJ Holt
- J Benito
- J Castresana
- J Castresana
- JK Park
- JL Boore
- Joerg Hetmank
- JR Lobry
- K Koike
- K Tomita
- KD Pruitt
- KL Tong
- KM Halanych
- L Pikó
- LA Frederico
- LH Hyman
- M Bernt
- M Bowmaker
- M Bulmer
- M Bulmer
- M Carullo
- M Nohara
- M Perseke
- M Perseke
- M Perseke
- Marleen Perseke
- Martin Schlegel
- Matthias Bernt
- MP Francino
- MY Yang
- NM Krishnan
- Peter F Stadler
- S Asakawa
- S Guindon
- S Matsuyama
- S Osawa
- S Yokobori
- S Yokoyama
- SE Massey
- SJ Bourlat
- T Sato
- T Stach
- T Yasukawa
- TA Brown
- TH Jukes
- TM Lowe
- V Ivanov
- VE Metschnikoff
- X Xia
- X Xia
- Y He
- Z Zhang
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>The Hemichordata comprises solitary-living Enteropneusta and colonial-living Pterobranchia, sharing morphological features with both Chordata and Echinodermata. Despite their key role for understanding deuterostome evolution, hemichordate phylogeny is controversial and only few molecular data are available for phylogenetic analysis. Furthermore, mitochondrial sequences are completely lacking for pterobranchs. Therefore, we determined and analyzed the complete mitochondrial genome of the pterobranch <it>Rhabdopleura compacta </it>to elucidate deuterostome evolution. Thereby, we also gained important insights in mitochondrial tRNA evolution.</p> <p>Results</p> <p>The mitochondrial DNA of <it>Rhabdopleura compacta </it>corresponds in size and gene content to typical mitochondrial genomes of metazoans, but shows the strongest known strand-specific mutational bias in the nucleotide composition among deuterostomes with a very GT-rich main-coding strand. The order of the protein-coding genes in <it>R. compacta </it>is similar to that of the deuterostome ground pattern. However, the protein-coding genes have been highly affected by a strand-specific mutational pressure showing unusual codon frequency and amino acid composition. This composition caused extremely long branches in phylogenetic analyses. The unusual codon frequency points to a selection pressure on the tRNA translation system to codon-anticodon sequences of highest versatility instead of showing adaptations in anticodon sequences to the most frequent codons. Furthermore, an assignment of the codon AGG to Lysine has been detected in the mitochondrial genome of <it>R. compacta</it>, which is otherwise observed only in the mitogenomes of some arthropods. The genomes of these arthropods do not have such a strong strand-specific bias as found in <it>R. compacta </it>but possess an identical mutation in the anticodon sequence of the tRNA<sub>Lys</sub>.</p> <p>Conclusion</p> <p>A strong reversed asymmetrical mutational constraint in the mitochondrial genome of <it>Rhabdopleura compacta </it>may have arisen by an inversion of the replication direction and adaptation to this bias in the protein sequences leading to an enigmatic mitochondrial genome. Although, phylogenetic analyses of protein coding sequences are hampered, features of the tRNA system of <it>R. compacta </it>support the monophyly of Ambulacraria. The identical reassignment of AGG to Lysine in two distinct groups may have occurred by convergent evolution in the anticodon sequence of the tRNA<sub>Lys</sub>.</p
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