171 research outputs found
Measurement of the top-quark mass in ttÂŻ events with dilepton final states in pp collisions at âs = 7 TeV
- Author
- Abbaneo D.
- Abbiendi G.
- Abbrescia M.
- Abdullin S.
- Abdulsalam A.
- Acosta D.
- Acosta J. G.
- Acosta M. Vazquez
- Adair A.
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Get PDFOpen Access: This article is distributed under the terms of the Creative Commons Attribution License.-- Chatrchyan, S. et al.The top-quark mass is measured in proton-proton collisions at sâ=7 TeV using a data sample corresponding to an integrated luminosity of 5.0 fbâ1 collected by the CMS experiment at the LHC. The measurement is performed in the dilepton decay channel ttÂŻâ(â+νâb)(ââν¯¯âbÂŻ), where â=e,Îź. Candidate top-quark decays are selected by requiring two leptons, at least two jets, and imbalance in transverse momentum. The mass is reconstructed with an analytical matrix weighting technique using distributions derived from simulated samples. Using a maximum-likelihood fit, the top-quark mass is determined to be 172.5Âą0.4 (stat.)Âą1.5 (syst.) GeV.Acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France);BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie program and the European Research Council (European Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von Humboldt Foundation; the Austrian Science Fund (FWF); the Belgian Federal Science Policy Office; the Fonds pour la Formation Ă la Recherche dans lâIndustrie et dans lâAgriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWTBelgium); the Ministry of Education, Youth and Sports (MEYS) of Czech Republic; the Council of Science and Industrial Research, India; the Compagnia di San Paolo (Torino); and the HOMING PLUS program of Foundation for Polish Science, cofinanced from European Union, Regional Development Fund.Peer Reviewe
Measurement of the t(t)over-bar production cross section in pp collisions at root s=7 TeV in dilepton final states containing a tau
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- Zito G
- Zotto P
- Zou W
- Zumerle G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe top quark pair production cross section is measured in dilepton events with one electron or muon, and one hadronically decaying tau lepton from the decay t (t) over bar -> (l nu(l))((sic)(h)nu((sic)))b (b) over bar, (l = e, mu). The data sample corresponds to an integrated luminosity of 2.0 fb(-1) for the electron channel and 2.2 fb(-1) for the muon channel, collected by the CMS detector at the LHC. This is the first measurement of the t (t) over bar cross section explicitly including tau leptons in proton- proton collisions at root s = 7 TeV. The measured value sigma(t (t) over bar) = 143 +/- 14(stat) +/- 22(syst) +/- 3(lumi) pb is consistent with the standard model predictions
Search for dijet resonances in 7 TeV pp collisions at CMS
- Author
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- Abbiendi G
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- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
Get PDFThis is the Pre-print version of the Article. The official published version of the paper can be accessed from the link below - Copyright @ 2010 APSA search for narrow resonances in the dijet mass spectrum is performed using data corresponding to an integrated luminosity of 2.9ââpb-1 collected by the CMS experiment at the Large Hadron Collider. Upper limits at the 95% confidence level are presented on the product of the resonance cross section, branching fraction into dijets, and acceptance, separately for decays into quark-quark, quark-gluon, or gluon-gluon pairs. The data exclude new particles predicted in the following models at the 95% confidence level: string resonances, with mass less than 2.50 TeV, excited quarks, with mass less than 1.58 TeV, and axigluons, colorons, and E6 diquarks, in specific mass intervals. This extends previously published limits on these models.This work is supported by FMSR (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); Academy of Sciences and NICPB (Estonia); Academy of Finland, ME, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); PAEC (Pakistan); SCSR (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MST and MAE (Russia); MSTD (Serbia); MICINN and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); TUBITAK and TAEK (Turkey); STFC (United Kingdom); DOE and NSF (USA)
Search for supersymmetry in events with b jets and missing transverse momentum at the LHC
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yilmaz Y
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- Zanetti M
- Zang J
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- Zumerle G
- Zuranski A
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2011
- Field of study
Get PDFA search for supersymmetry is presented using a sample of events with b jets and missing transverse momentum. The search uses a data sample of proton-proton collisions at a centre-of-mass energy of 7TeV, corresponding to an integrated luminosity of 35 pb(-1), collected with the CMS detector. A total of 0.33(-0.33)(+0.43) (stat.) +/- 0.13 (syst.) events is predicted, using control samples in the data, to arise from standard model processes, and one event is observed in the data. Upper limits are set at the 95% confidence level on the cross sections of benchmark supersymmetric models
Indications of suppression of excited ÎĽ states in Pb-Pb collisions at âsNN = 2.76TeV
- Author
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- Zoeller MH
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Get PDFThis is the pre-print version of the Published Article which can be accessed from the link below.A comparison of the relative yields of ÎĽ resonances in the Îź+Îź- decay channel in Pb-Pb and pp collisions at a center-of-mass energy per nucleon pair of 2.76 TeV is performed with data collected with the CMS detector at the LHC. Using muons of transverse momentum above 4ââGeV/c and pseudorapidity below 2.4, the double ratio of the ÎĽ(2S) and ÎĽ(3S) excited states to the ÎĽ(1S) ground state in Pb-Pb and pp collisions, [ÎĽ(2S+3S)/ÎĽ(1S)]Pb-Pb/[ÎĽ(2S+3S)/ÎĽ(1S)]pp, is found to be 0.31-0.15+0.19(stat)Âą0.03(syst). The probability to obtain the measured value, or lower, if the true double ratio is unity, is calculated to be less than 1%
Long-range and short-range dihadron angular correlations in central PbPb collisions at âsNN=2.76 TeV
- Author
- Abbaneo D
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdullin S
- Acosta D
- Acosta D
- Acosta JG
- Acosta MV
- Acosta MV
- Adam N
- Adam W
- Adams MR
- Adams MR
- Adams T
- Adams T
- Adiguzel A
- Adiguzel A
- Adler V
- Adzic P
- Adzic P
- Afanasiev S
- Afanasiev S
- Agostino L
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilar-Benitez M
- Aguilo E
- Aguilo E
- Ahmad M
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Akgun B
- Akgun U
- Akgun U
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- Civinini C
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- Ingram Q
- Innocente V
- Innocente V
- Iorio AOM
- Isildak B
- Isildak B
- Issah M
- Ivanov A
- Ivanov Y
- Ivanov Y
- Jabeen S
- Jabeen S
- Jackson J
- Jackson J
- Jafari A
- Jain S
- Jain S
- Jain S
- Jang DW
- Jang DW
- Janot P
- Janot P
- Janssen X
- Janulis M
- Janulis M
- Jarrin EC
- Jarrin EC
- Jarry P
- Jarvis C
- Jarvis C
- Jarvis M
- Jeitler M
- Jeng GY
- Jeng GY
- Jenkins M
- Jenkins M
- Jensen H
- Jensen H
- Jeong C
- Jeong MS
- Jeong MS
- Jessop C
- Jiang CH
- Jindal M
- Jindal P
- Jo M
- Jo M
- Johns W
- Johnson KF
- Johnson KF
- Johnson M
- Johnson M
- Jones J
- Jones M
- Jorda C
- Jorda C
- Josa MI
- Josa MI
- Joshi U
- Joshi U
- Juillot P
- Jun SY
- Jun SY
- Jung H
- Jussen R
- Justus C
- Justus C
- Kaadze K
- Kaadze K
- Kachanov V
- Kachanov V
- Kadastik M
- Kadija K
- Kaestli HC
- Kaestli HC
- Kaftanov V
- Kaftanovy V
- Kailas S
- Kalakhety H
- Kalakhety H
- Kalavase P
- Kalavase P
- Kalinowski A
- Kalinowski A
- Kalogeropoulos A
- Kamenev A
- Kamenev A
- Kamon T
- Kang S
- Kang S
- Kangal EE
- Kangal EE
- Kao KY
- Kao KY
- Kao SC
- Kao SC
- Kapusi A
- Karadzhinova A
- Karaman T
- Karapostoli G
- Karapostoli G
- Karavakis E
- Karavakis E
- Karchin PE
- Karim M
- Karimaki V
- Karjavin V
- Karjavin V
- Karmgard DJ
- Kaschube K
- Kasemann M
- Katkov I
- Katsas P
- Kaufman GN
- Kaufman GN
- Kaur M
- Kaussen G
- Kaya M
- Kaya M
- Kaya O
- Kaya O
- Kazana M
- Kazana M
- Keller J
- Kelley R
- Kelley R
- Kellogg RG
- Kelly T
- Kennedy BW
- Kennedy BW
- Kesisoglou S
- Khachatryan V
- Khakzad M
- Khalatyan S
- Khalatyan S
- Khalil S
- Khalil S
- Khan A
- Khan A
- Khan WA
- Khan WA
- Kharchilava A
- Khatiwada R
- Khatiwada R
- Khotilovich V
- Khukhunaishvili A
- Khukhunaishvili A
- Khurana R
- Khurshid T
- Khurshid T
- Kiesenhofer W
- Killewald P
- Kim B
- Kim B
- Kim DH
- Kim DH
- Kim GN
- Kim GN
- Kim H
- Kim H
- Kim H
- Kim H
- Kim JE
- Kim JE
- Kim JH
- Kim JH
- Kim JY
- Kim JY
- Kim MS
- Kim MS
- Kim TJ
- Kim TJ
- Kim V
- Kim V
- Kim Y
- Kim Z
- Kim Z
- Kinnunen R
- Kirakosyan M
- Kirakosyan M
- Kirn M
- Kirsanov M
- Kirsanov M
- Klabbers P
- Klanner R
- Klapoetke K
- Klein B
- Klein K
- Kleinwort C
- Klima B
- Klima B
- Klimkovich T
- Klingebiel D
- Kluge H
- Klukas J
- Klute M
- Klyukhin V
- Knutsson A
- Ko W
- Ko W
- Koay SA
- Koay SA
- Kodolova O
- Kodolova O
- Kohli JM
- Kokkas P
- Kolb J
- Kolberg T
- Komaragiri JR
- Konecki M
- Konecki M
- Kong DJ
- Kong DJ
- Konig S
- Konigsberg J
- Konigsberg J
- Konstantinov D
- Konstantinov D
- Kopecky A
- Kopecky A
- Korablev A
- Korablev A
- Korotkikh V
- Korpela A
- Kortelainen MJ
- Korytov A
- Korytov A
- Kossov M
- Kossovl M
- Kotlinski D
- Kotlinski D
- Kotov K
- Kousouris K
- Kousouris K
- Kovalskyi D
- Kovalskyi D
- Kovitanggoon K
- Koybasi O
- Kozhuharov V
- Kozlov G
- Kozlov G
- Kraan A
- Krajczar K
- Kramer L
- Kramer L
- Kramer M
- Krammer M
- Krasnikov N
- Krasnikov N
- Kravchenko I
- Kreczko L
- Kreczko L
- Kreis B
- Kreis B
- Kress M
- Kress T
- Kreuzer P
- Kroeger R
- Krofcheck D
- Krofcheck D
- Krokhotin A
- Krokhotin A
- Krolikowski J
- Krolikowski J
- Kropivnitskaya A
- Kropivnitskaya A
- Krpic D
- Krpic D
- Krucker D
- Krutelyov V
- Krutelyov V
- Krychkine V
- Krychkine V
- Kubik A
- Kubota Y
- Kuessel Y
- Kuhr T
- Kukartsev G
- Kukartsev G
- Kumar A
- Kumar A
- Kumar V
- Kunde GJ
- Kunde GJ
- Kunori S
- Kunori S
- Kuo CM
- Kuo CM
- Kurca T
- Kurt P
- Kuznetsova E
- Kwan S
- Kwan S
- Kwon E
- Kwon E
- Kyberd P
- Kyberd P
- Kypreos T
- Kypreos T
- Kyriakis A
- Laasanen AT
- Lacaprara S
- Lacroix F
- Lacroix F
- Lae CK
- Lae CK
- Lagana C
- Laird E
- Lamichhane P
- Lampen T
- Lanaro A
- Lander R
- Lander R
- Landsberg G
- Landsberg G
- Lanev A
- Lanev A
- Lange D
- Lange J
- Lange W
- Langenegger U
- Langenegger U
- Lannon K
- Lanske D
- Lariccia P
- Lassila-Perini K
- Lath A
- Lawson P
- Lawson P
- Lazaridis C
- Lazic D
- Lazic D
- Lazo-Flores J
- Lazzizzera I
- Le Bihan AC
- Le Grand T
- Lebolo LM
- Lebolo LM
- Lebourgeois M
- Lebourgeois M
- Lecomte P
- Lecomte P
- Lecoq P
- Lecoq P
- Ledovskoy A
- Lee J
- Lee J
- Lee KS
- Lee KS
- Lee S
- Lee S
- Lee SW
- Lee YJ
- Lehti S
- Lei YJ
- Lei YJ
- Lelas D
- Lelas K
- Lellouch J
- Lemaitre V
- Lenzi P
- Leonard J
- Leonardo N
- Leonidopoulos C
- Leonidopoulos C
- Leonidov A
- Leonidov A
- Leslie D
- Leslie D
- Lethuillier M
- Letts J
- Letts J
- Levchenko P
- Levchenko P
- Levchuk L
- Levchuk L
- Li SW
- Li SW
- Li W
- Li W
- Liang D
- Liang S
- Liao J
- Ligabue F
- Liko D
- Limon P
- Limon P
- Lin C
- Lin W
- Lin W
- Linares EC
- Linares EC
- Lincoln D
- Lincoln D
- Linden T
- Ling TY
- Linn A
- Linn S
- Linn S
- Lipton R
- Lipton R
- Lista L
- Litov L
- Liu C
- Liu F
- Liu F
- Liu H
- Liu H
- Liu H
- Liu H
- Liu H
- Liu MH
- Liu YF
- Liu YF
- Liu ZK
- Liu ZK
- Llatas M
- Llatas MC
- Locci E
- Lohmann W
- Loizides C
- Lokhtin I
- Lokhtin I
- Lomidze D
- Lomtadze T
- Long OR
- Long OR
- Longo E
- Lopez A
- Lopez EL
- Lopez EL
- Lopez OG
- Lopez OG
- Lopez SG
- Lopez SG
- Lopez-Fernandez R
- Lopez-Fernandez R
- Loukas D
- Lourenco C
- Lourenco C
- Loveless R
- Lowette S
- Lowette S
- Lu RS
- Lu RS
- Lu Y
- Lu YJ
- Lu YJ
- Lucaroni A
- Luckey PD
- Luk M
- Lungu G
- Luo W
- Lusito L
- Lustermann W
- Lustermann W
- Luthra A
- Luthra A
- Luukka P
- Lychkovskaya N
- Lychkovskaya N
- Lykken J
- Lykken J
- Lynch S
- Lyons L
- Lyons L
- Ma T
- Ma Y
- Ma Y
- MacEvoy BC
- MacEvoy BC
- Maenpaa T
- Maes J
- Maes M
- Maes T
- Maeshima K
- Maeshima K
- Maestre JA
- Maestre JA
- Magass C
- Maggi G
- Maggi M
- Magnan AM
- Magnan AM
- Maguire C
- Mahmoud MA
- Maity M
- Majumder D
- Majumder G
- Maki T
- Maki T
- Makouski M
- Maksimovic P
- Malberti M
- Malbouisson H
- Malcles J
- Malek M
- Malek M
- Malgeri L
- Malgeri L
- Malik S
- Malik S
- Malvezzi S
- Mane P
- Mangano B
- Mangano B
- Mankel R
- Manna N
- Mannelli M
- Mannelli M
- Manolakos I
- Mans J
- Manthos N
- Mantovani G
- Mao Y
- Marage PE
- Marangelli B
- Maravin Y
- Marcellini S
- Marchica C
- Marchica C
- Marco J
- Marco J
- Marco R
- Marco R
- Margoni M
- Marienfeld M
- Marinelli N
- Marinho F
- Marinov A
- Marionneau M
- Mariotti C
- Markina A
- Markou A
- Markou C
- Markowitz P
- Markowitz P
- Marlow D
- Maron G
- Marone M
- Maroussov V
- Marraffino JM
- Marraffino JM
- Marrouche J
- Marrouche J
- Martelli A
- Martin MA
- Martin W
- Martin W
- Martinez G
- Martinez G
- Martini L
- Martins CD
- Martisiute D
- Martisiute D
- Martschei D
- Maruyama S
- Maruyama S
- Maselli S
- Masetti G
- Masetti L
- Masetti L
- Mason D
- Mason D
- Massironi A
- Matchev K
- Matchev K
- Mateev M
- Mathias B
- Matorras F
- Matorras F
- Mattson M
- Matveev V
- Matveev V
- Maurisset A
- Mavrommatis C
- Mazumdar K
- McBride P
- McBride P
- Mccartin J
- McCliment E
- McCliment E
- Mccoll N
- Mccoll N
- Medvedeva T
- Mehdiabadi SP
- Mehta MZ
- Mehta P
- Meier F
- Meier F
- Meijers F
- Meijers F
- Mejias BM
- Mejias BM
- Mekterovic D
- Mekterovic D
- Melo A
- Melzer-Pellmann IA
- Menasce D
- Mendez H
- Meneghelli M
- Meneguzzo AT
- Menendez JF
- Menendez JF
- Meng X
- Menichelli M
- Mercadante PG
- Mercier D
- Meridiani P
- Meridiani P
- Merino G
- Merino G
- Merkel P
- Merlo JP
- Merlo JP
- Mermerkaya H
- Mermerkaya H
- Merola M
- Merschmeyer M
- Mersi S
- Mersi S
- Mertzimekis TJ
- Merz J
- Mesa D
- Mesa D
- Meschi E
- Meschi E
- Meschini M
- Mesropian C
- Messineo A
- Mestvirishvili A
- Mestvirishvili A
- Metson S
- Metson S
- Meyer A
- Meyer AB
- Miao T
- Miao T
- Miceli T
- Miceli T
- Migliore E
- Mignerey AC
- Mikami Y
- Mikulec I
- Mila G
- Milenovic P
- Milenovic P
- Militaru O
- Miller DH
- Millischer L
- Milosevic J
- Milosevic J
- Milstene C
- Mine P
- Miner DC
- Mirabito L
- Mironov C
- Mishra K
- Mishra K
- Mitselmakher G
- Mitselmakher G
- Mnich J
- Moeller A
- Moeller A
- Mohammadi A
- Mohanty AK
- Mohanty GB
- Mohapatra A
- Mohr N
- Moisenz P
- Moisenz P
- Molnar J
- Monaco V
- Mondal NK
- Montalvo R
- Montanari A
- Montanino D
- Montanino D
- Montoya CAC
- Moon DH
- Moon DH
- Mooney M
- Moortgat F
- Moortgat F
- Moreno BG
- Moreno SC
- Moreno SC
- Moroni L
- Morovic S
- Morse DM
- Moser R
- Moser R
- Mossolov V
- Mott A
- Mott A
- Mousa J
- Mozer MU
- Mozer MU
- Mrenna S
- Mrenna S
- Mucibello L
- Mueller S
- Mulders M
- Mulders M
- Muller T
- Mundim L
- Muniz L
- Muniz L
- Muntel M
- Mura B
- Murray M
- Murzin V
- Murzin V
- Musella P
- Musella P
- Musenich R
- Musich M
- Musienko Y
- Musienko Y
- Mussgiller A
- My S
- Nachtman J
- Nachtman J
- Nageli C
- Nahn S
- Naimuddin M
- Najafabadi MM
- Nam SK
- Nam SK
- Nandi R
- Nandi R
- Nappi A
- Narain M
- Narain M
- Nart A
- Nash J
- Nash J
- Nauenberg U
- Nauenberg U
- Naumann-Emme S
- Navarria FL
- Nawrocki K
- Nawrocki K
- Nayak A
- Nayak A
- Nef P
- Nef R
- Nespolo M
- Nessi-Tedaldi F
- Nessi-Tedaldi F
- Nesvold E
- Nesvold E
- Neu C
- Neumeister N
- Newbold DM
- Newbold DM
- Newman HB
- Newman HB
- Newman-Holmes C
- Newman-Holmes C
- Newsom CR
- Newsom CR
- Nguyen D
- Nguyen D
- Nguyen H
- Nguyen H
- Nguyen M
- Nguyen M
- Nicolaou C
- Niegel M
- Nikitenko A
- Nikitenko A
- Nikolic M
- Nikolic M
- Nirunpong K
- Nirunpong K
- Nishu N
- Nogima H
- Noonan D
- Norbeck E
- Norbeck E
- Nourbakhsh S
- Novaes SF
- Nowack A
- Nowak F
- Ntomari E
- Nuzzo S
- O'Brien C
- O'Brien C
- O'Dell V
- O'Dell V
- Oberst O
- Obertino MM
- Obraztsov S
- Obraztsov S
- Ocalan K
- Ocalan K
- Ochando C
- Ochesanu S
- Odell N
- Odorici F
- Oehler A
- Oguri V
- Olaiya E
- Olaiya E
- Oliveros AFO
- Oliveros S
- Olsen J
- Olson J
- Olson J
- Olzem J
- Onel Y
- Onel Y
- Onen JHA
- Onengut G
- Onengut G
- Onig SK
- Orbaker D
- Oreshkin V
- Oreshkin V
- Organtini G
- Orimoto T
- Orimoto T
- Orsini L
- Orsini L
- Osipenkov I
- Ostapchuk A
- Otiougova P
- Otiougova P
- Ott J
- Ovyn S
- Ozdemir K
- Ozdemir K
- Ozkorucuklu S
- Ozkorucuklu S
- Ozok F
- Ozok F
- Ozpineci A
- Ozpineci A
- Ozturk S
- Ozturk S
- Pacifico N
- Padhi S
- Padhi S
- Padley BP
- Padula SS
- Paganini P
- Pagano D
- Paganoni M
- Pakhotin Y
- Pakhotin Y
- Palichik V
- Palichik V
- Palinkas J
- Palla F
- Palmer C
- Palmer C
- Palmonari F
- Panagiotou A
- Pandolfi F
- Pant LM
- Panwalkar S
- Paoletti S
- Paolucci P
- Papacz P
- Papadopoulos I
- Papageorgiou A
- Papageorgiou A
- Pape L
- Pape L
- Paramatti R
- Parashar N
- Pardo PL
- Pardo PL
- Pardos CD
- Pardos CD
- Park C
- Park C
- Park H
- Park H
- Park IC
- Park IC
- Park S
- Park S
- Park SK
- Park SK
- Parracho PGF
- Parracho PGF
- Pashenkov A
- Pashenkov A
- Passaseo M
- Pastrone N
- Patel R
- Patras V
- Patterson JR
- Patterson JR
- Paulini M
- Paulini M
- Paus C
- Pauss F
- Pauss F
- Pavlov B
- Pavlunin V
- Pavlunin V
- Pearson T
- Pedrini D
- Pegna DL
- Peiffer T
- Pelayo JP
- Pellett D
- Pellett D
- Pelliccioni M
- Pelliccioni M
- Pens AD
- Penzo A
- Penzo A
- Perchalla L
- Pereira AV
- Pereira AV
- Perelygin V
- Perelygin V
- Perera L
- Perez E
- Perez E
- Perez JAC
- Perez JAC
- Perfilov M
- Perieanu A
- Peris AD
- Pernicka M
- Perries S
- Perrotta A
- Perrozzi L
- Pesaresi M
- Pesaresi M
- Petkov P
- Petrakou E
- Petridis K
- Petridis K
- Petrilli A
- Petrilli A
- Petrillo G
- Petrov P
- Petrov P
- Petrov V
- Petrov V
- Petrucciani G
- Petrucciani G
- Petrushanko S
- Petyt D
- Petyt D
- Pfeiffer A
- Pfeiffer A
- Pi H
- Pi H
- Piccolo D
- Pieri M
- Pieri M
- Pierini M
- Pierini M
- Pierro GA
- Pieta H
- Pietsch N
- Pimia M
- Pimia M
- Pin A
- Pineda AM
- Pineda AM
- Pioppi M
- Pioppi M
- Piotrzkowski K
- Piparo D
- Piperov S
- Piroue P
- Pitzl D
- Pivarski J
- Plager C
- Plager C
- Plestina R
- Pol ME
- Polatoz A
- Polatoz A
- Polese G
- Polese G
- Polic D
- Poll A
- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popov V
- Popov V
- Pordes R
- Pordes R
- Pozdnyakov A
- Pozzobon N
- Prescott C
- Prescott C
- Primavera F
- Prokofyev O
- Prokofyev O
- Prosper H
- Prosper H
- Ptochos F
- Puerta J
- Pugliese G
- Puigh D
- Puigh D
- Puljak I
- Punz T
- Punz T
- Qazi S
- Qazi S
- Qian SJ
- Quan X
- Quast G
- Quertenmont L
- Quertenmont L
- Rabbertz K
- Racz A
- Racz A
- Radburn-Smith BC
- Radburn-Smith BC
- Ragazzi S
- Rahatlou S
- Rahmat R
- Raics P
- Raidal M
- Rakness G
- Rakness G
- Ralich R
- Ralich R
- Ralph D
- Ramos JPF
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- Rander J
- Ranieri R
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- Ranjan K
- Rappoccio S
- Raspereza A
- Ratnikov F
- Ratnikova N
- Ratti SP
- Raupach F
- Raval A
- Ray EAF
- Raymond DM
- Raymond DM
- Razis PA
- Rebane L
- Rebassoo F
- Rebassoo F
- Redaelli N
- Redjimi R
- Redondo I
- Reeder D
- Regenfus C
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- Reid ID
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- Reithler H
- Rekovic V
- Remington R
- Remington R
- Renker D
- Renker D
- Rennefeld J
- Renz M
- Reucroft S
- Reyes-Santos MA
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- Rhee HB
- Rhee HB
- Ribeiro PQ
- Ribnik J
- Ribnik J
- Riccardi C
- Richards A
- Richman J
- Richman J
- Rikova MI
- Rikova MI
- Rios AAO
- Rivero CM
- Rivero CM
- Rizzi A
- Rizzi A
- Ro SR
- Ro SR
- Roberts J
- Robles J
- Robles J
- Robmann P
- Robmann P
- Rodenburg M
- Rodozov M
- Rodrigo T
- Rodrigo T
- Rodriguez JL
- Rodriguez JL
- Rodriguez-Marrero AY
- Rodriguez-Marrero AY
- Rogan C
- Rogan C
- Rogerson S
- Roh Y
- Rohe T
- Rohe T
- Rohlf J
- Rohlf J
- Rohringer H
- Roland B
- Roland C
- Roland G
- Rolandi G
- Rolandi G
- Romano F
- Romanowska-Rybinska K
- Romanowska-Rybinska K
- Romeo F
- Romero A
- Romero A
- Romero L
- Romero L
- Rommerskirchen T
- Rommerskirchen T
- Rompotis N
- Rompotis N
- Ronchese P
- Ronga FJ
- Ronga FJ
- Rose A
- Rose A
- Rose K
- Roselli G
- Rosin M
- Rosowsky A
- Ross I
- Rossato K
- Rossi AM
- Rossin R
- Rossin R
- Rossini M
- Rossini M
- Rougny R
- Rovelli C
- Rovelli C
- Rovelli T
- Rovere M
- Rovere M
- Ruchti R
- Rudolph M
- Ruiz-Jimeno A
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Rusakov SV
- Rusakov SV
- Ruspa M
- Ruspa M
- Russ J
- Russ J
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- Ryckbosch D
- Ryd A
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- Ryu G
- Ryu G
- Ryutin R
- Ryutin R
- Sabes D
- Sabonis T
- Sabonis T
- Sacchi R
- Sacchi R
- Safarzadeh B
- Safonov A
- Safronov G
- Safronov G
- Saha A
- Saini LK
- Saka H
- Sakharov A
- Sakulin H
- Sakulin H
- Sala L
- Sala L
- Sala S
- Salerno R
- Salur S
- Salur S
- Salvati E
- Sammet J
- Sanabria JC
- Sanchez AK
- Sanchez AK
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- Sanchez FJM
- Sanchez JG
- Sanchez JG
- Sanchez MCD
- Sanchez MCD
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- Sanchez-Hernandez A
- Sander C
- Sanders DA
- Sanders S
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- Sani M
- Santanastasio F
- Santaolalla J
- Santaolalla J
- Santocchia A
- Santoro A
- Sanudo MS
- Sanudo MS
- Saoulidou N
- Saoulidou N
- Saout C
- Sarycheva L
- Sarycheva L
- Sasseville M
- Sauerland P
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- Sawley MC
- Sawley MC
- Schael S
- Schafer C
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- Schettler H
- Scheurer A
- Schieferdecker P
- Schilling FP
- Schlein P
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- Schleper P
- Schmidt A
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- Schmidt R
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- Schnetzer S
- Schoerner-Sadenius T
- Schofbeck R
- Schott G
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- Zoeller MH
- Zorbilmez C
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2011
- Field of study
Get PDFThis is the pre-print version of the Published Article, which can be accessed from the link below.First measurements of dihadron correlations for charged particles are presented
for central PbPb collisions at a nucleon-nucleon center-of-mass energy of 2.76TeV over a broad range in relative pseudorapidity ( ) and the full range of relative azimuthal angle ( ). The data were collected with the CMS detector, at the LHC. A broadening of the away-side ( ) azimuthal correlation is observed at all , as compared to the measurements in pp collisions. Furthermore, long-range dihadron correlations in are observed for particles with similar values. This phenomenon, also known as the \ridge",
persists up to at least j j = 4. For particles with transverse momenta (pT) of 2-4 GeV/c, the ridge is found to be most prominent when these particles are correlated with particles of pT = 2-6 GeV/c, and to be much reduced when paired with particles of pT = 10-12 GeV/c
Measurement of the t-channel single top quark production cross section in pp collisions at âs = 7TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Zoeller MH
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- Zumerle G
- Zuranski A
- Publication venue
- American Physical Society
- Publication date
- 01/01/2011
- Field of study
Get PDFThis is the pre-print version of the Published Article which can be accessed from the link below.Electroweak production of the top quark is measured for the first time in pp collisions at âs=7ââTeV, using a data set collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 36ââpb-1. With an event selection optimized for t-channel production, two complementary analyses are performed. The first one exploits the special angular properties of the signal, together with background estimates from the data. The second approach uses a multivariate analysis technique to probe the compatibility with signal topology expected from electroweak top-quark production. The combined measurement of the cross section is 83.6Âą29.8(stat+syst)Âą3.3(lumi)ââpb, consistent with the standard model expectation
Dijet azimuthal decorrelations in pp collisions at âs = 7TeV
- Author
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- Yi K
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- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
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- 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
- American Physical Society
- Publication date
- 01/01/2011
- Field of study
Get PDFThis is the pre-print version of the Published Article which can be accessed from the link below.Measurements of dijet azimuthal decorrelations in pp collisions at âs=7ââTeV using the CMS detector at the CERN LHC are presented. The analysis is based on an inclusive dijet event sample corresponding to an integrated luminosity of 2.9ââpb-1. The results are compared to predictions from perturbative QCD calculations and various Monte Carlo event generators. The dijet azimuthal distributions are found to be sensitive to initial-state gluon radiation
Measurement of the inclusive jet cross section in pp collisions at âs = 7TeV
- Author
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- Zanetti M
- Zang J
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- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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- 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
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Get PDFThis is the pre-print version of the Published Article which can be accessed from the link below.The inclusive jet cross section is measured in pp collisions with a center-of-mass energy of 7 TeV at the Large Hadron Collider using the CMS experiment. The data sample corresponds to an integrated luminosity of 34ââpb-1. The measurement is made for jet transverse momenta in the range 18â1100 GeV and for absolute values of rapidity less than 3. The measured cross section extends to the highest values of jet pT ever observed and, within the experimental and theoretical uncertainties, is generally in agreement with next-to-leading-order perturbative QCD predictions
Search for same-sign top-quark pair production at root s=7 TeV and limits on flavour changing neutral currents in the top sector
- 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
- Afanasiev S
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahmed I
- 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
- Antonelli L
- Antunes JR
- Antunovic Z
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- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
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- Azzolini V
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- Baarmand MM
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- Bakirci MN
- Bakken JA
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- Banerjee S
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- Bani L
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2011
- Field of study
Get PDFAn inclusive search for same-sign top-quark pair production in pp collisions at root s = 7 TeV is performed using a data sample recorded with the CMS detector in 2010, corresponding to an integrated luminosity of 35 pb(-1). This analysis is motivated by recent studies of p (p) over bar -> t (t) over bar reporting mass-dependent forward-backward asymmetries larger than expected from the standard model. These asymmetries could be due to Flavor Changing Neutral Currents (FCNC) in the top sector induced by t -channel exchange of a massive neutral vector boson (Z'). Models with such a Z' also predict enhancement of same-sign top-pair production in pp or pp collisions. Limits are set as a function of the Z' mass and its couplings to u and t quarks. These limits disfavour the FCNC interpretation of the Tevatron results
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