474 research outputs found
Disrupted postnatal lung development in heme oxygenase-1 deficient mice
- Author
- A Jozkowicz
- A Yachie
- AM Choi
- B Bussolati
- B Thebaud
- BB Warner
- BM Deramaudt
- D Massaro
- D Massaro
- D Massaro
- D Massaro
- D Warburton
- DG Grier
- F Groenman
- GD Massaro
- GD Massaro
- GD Massaro
- GT Wagenaar
- H Zhou
- HJ Duckers
- J Dulak
- JD Merrill
- JL Emery
- KD Poss
- KD Poss
- KJ Barrington
- LB Clerch
- LE Otterbein
- M Maden
- M Tsoumakidou
- MD Maines
- MP Soares
- N Li
- NG Abraham
- PA Dennery
- PA Dennery
- PA Dennery
- R Stocker
- RL Auten
- S Dore
- S Friedman
- S Mumby
- T Minamino
- T Morita
- T Yoshida
- T Yoshinaga
- TB Deramaudt
- TP Cooney
- Y Lavrovsky
- YH Weng
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Do Electronic Health Records Help or Hinder Medical Education?
- Author
- Publication venue
- Public Library of Science
- Publication date
- 01/05/2009
- Field of study
Many countries worldwide are digitizing patients' medical records. What impact will these electronic health records have upon medical education? This debate examines the threats and opportunities
Restricted Attentional Capacity within but Not between Sensory Modalities: An Individual Differences Approach
- Author
- A Larsen
- AM Bonnel
- AM Treisman
- AP Hillstrom
- CD Wickens
- CNL Olivers
- D Alais
- DA Allport
- DW Massaro
- E Tulving
- E van der Burg
- G Hein
- HE Egeth
- J Duncan
- J Long
- JA Swets
- JE Raymond
- John Duncan
- K Shapiro
- KK Evans
- KM Arnell
- KM Arnell
- KM Arnell
- KM Arnell
- KM Arnell
- Manasa Kandula
- Matthieu Louis
- MC Potter
- MC Potter
- MH Giard
- MM Chun
- MM Taylor
- NA Taatgen
- P Jolicoeur
- R Dell'Acqua
- RM Shiffrin
- S Martens
- S Martens
- S Martens
- S Martens
- S Martens
- S Soto-Faraco
- Sander Martens
- SJ Luck
- W Schneider
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Background Most people show a remarkable deficit to report the second of two targets when presented in close temporal succession, reflecting an attentional blink (AB). An aspect of the AB that is often ignored is that there are large individual differences in the magnitude of the effect. Here we exploit these individual differences to address a long-standing question: does attention to a visual target come at a cost for attention to an auditory target (and vice versa)? More specifically, the goal of the current study was to investigate a) whether individuals with a large within-modality AB also show a large cross-modal AB, and b) whether individual differences in AB magnitude within different modalities correlate or are completely separate. Methodology/Principal Findings While minimizing differential task difficulty and chances for a task-switch to occur, a significant AB was observed when targets were both presented within the auditory or visual modality, and a positive correlation was found between individual within-modality AB magnitudes. However, neither a cross-modal AB nor a correlation between cross-modal and within-modality AB magnitudes was found. Conclusion/Significance The results provide strong evidence that a major source of attentional restriction must lie in modality-specific sensory systems rather than a central amodal system, effectively settling a long-standing debate. Individuals with a large within-modality AB may be especially committed or focused in their processing of the first target, and to some extent that tendency to focus could cross modalities, reflected in the within-modality correlation. However, what they are focusing (resource allocation, blocking of processing) is strictly within-modality as it only affects the second target on within-modality trials. The findings show that individual differences in AB magnitude can provide important information about the modular structure of human cognition
Impact of stroke unit in a public hospital on length of hospitalization and rate of early mortality of ischemic stroke patients
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
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
- Olsen J
- Ong R. A.
- Ongmongkolkul P
- Onorato G
- Onuchin AP
- Orr M.
- Otte A. N.
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Paoloni E
- Park N.
- Park W
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pegna DL
- Peimer DR
- Perez A
- Perkins J. S.
- Perl M
- Perlman E. S.
- Peruzzi IM
- Piccolo M
- Pichel A.
- Piemontese L
- Piredda G
- Playfer S
- Pohl M.
- Poireau V
- Porter FC
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prepost R
- 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+eââJ/ÏÏ+Ïâ 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
fbâ1. We investigate the J/ÏÏ+Ïâ mass
distribution in the region from 3.5 to 5.5 GeV/c2. Below 3.7
GeV/c2 the Ï(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 114â15+16â (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 Ï+Ïâ system
which results from Y(4260) decay
Search for Charged Higgs Bosons in e+e- Collisions at \sqrt{s} = 189 GeV
- Author
- Acciarri M
- Achard P
- Adriani O
- Aguilar-Benitez M
- Alcaraz J
- Alemanni G
- Allaby J
- Aloisio A
- Alviggi MG
- Ambrosi G
- Anderhub H
- Andreev VP
- Angelescu T
- Anselmo F
- Arefiev A
- Azemoon T
- Aziz T
- Bagnaia P
- Baksay L
- Balandras A
- Ball RC
- Banerjee S
- Banerjee S
- Barczyk A
- Barillere R
- Barone L
- Bartalini P
- Basile M
- Battiston R
- Bay A
- Becattini F
- Becker U
- Behner F
- Bellucci L
- Berdugo J
- Berges P
- Bertucci B
- Betev BL
- Bhattacharya S
- Biasini M
- Biland A
- Blaising JJ
- Blyth SC
- Bobbink GJ
- Bohm A
- Boldizsar L
- Borgia B
- Bourilkov D
- Bourquin M
- Bourquin M
- Braccini S
- Braccini S
- Branson JG
- Branson JG
- Brigljevic V
- Brigljevic V
- Brochu F
- Brochu F
- Buffini A
- Buijs A
- Burger JD
- Burger WJ
- Busenitz J
- Button A
- Cai XD
- Campanelli M
- Capell M
- Carlino G
- Cartacci AM
- Casaus J
- Castellini G
- Cavallari F
- Cavallo N
- Cecchi C
- Cerrada M
- Cesaroni F
- Chamizo M
- Chang YH
- Chaturvedi UK
- Chemarin M
- Chen A
- Chen G
- Chen GM
- Chen HF
- Chen HS
- Chereau X
- Chiefari G
- Cifarelli L
- Cindolo F
- Civinini C
- Clare I
- Clare R
- Coignet G
- Colijn AP
- Colino N
- Costantini S
- Cotorobai F
- Cozzoni B
- Csilling A
- Cucciarelli S
- D'Alessandro R
- Dai TS
- de Asmundis R
- de Guevara PL
- de Jong P
- de la Cruz B
- De Notaristefani F
- De Salvo A
- Deglon P
- Degre A
- Deiters K
- della Volpe D
- Denes P
- Di Lodovico F
- Diemoz M
- Dionisi C
- Dittmar M
- Dominguez A
- Doria A
- Dova MT
- Duchesneau D
- Dufournaud D
- Duinker P
- Duran I
- El Mamouni H
- Engler A
- Eppling FJ
- Erne FC
- Extermann P
- Fabre M
- Faccini R
- Falagan MA
- Falciano S
- Favara A
- Fay J
- Fedin O
- Felcini M
- Ferguson T
- Ferroni F
- Fesefeldt H
- Fiandrini E
- Field JH
- Filthaut F
- Fisher PH
- Fisk I
- Forconi G
- Fredj L
- Freudenreich K
- Furetta C
- Galaktionov Y
- Ganguli SN
- Garcia-Abia P
- Gataullin M
- Gau SS
- Gentile S
- Gheordanescu N
- Giagu S
- Gong ZF
- Grenier G
- Grimm O
- Gruenewald MW
- Guida M
- Gupta VK
- Gurtu A
- Gutay LJ
- Haas D
- Hasan A
- Hatzifotiadou D
- Hebbeker T
- Herve A
- Hidas P
- Hirschfelder J
- Hofer H
- Holzner G
- Hoorani H
- Hou SR
- Iashvili I
- Jin BN
- Jones LW
- Josa-Mutuberria I
- Kamrad D
- Kaur M
- Khan RA
- Kienzle-Focacci MN
- Kim D
- Kim DH
- Kim JK
- Kim SC
- Kirkby J
- Kiss D
- Kittel W
- Klimentov A
- Konig AC
- Kopp A
- Korolko I
- Koutsenko V
- Kraber M
- Kraemer RW
- Krenz W
- Kunin A
- Laktineh I
- Landi G
- Lassila-Perini K
- Laurikainen P
- Lavorato A
- Le Coultre P
- Le Goff JM
- Lebeau M
- Lebedev A
- Lebrun P
- Lecomte P
- Lecoq P
- Lee HJ
- Leiste R
- Leonardi E
- Levtchenko P
- Li C
- Lin CH
- Lin WT
- Linde FL
- Lista L
- Liu ZA
- Lohmann W
- Longo E
- Lu YS
- Lubelsmeyer K
- Luci C
- Luckey D
- Lugnier L
- Luminari L
- Lustermann W
- Ma WG
- Maity M
- Malgeri L
- Malinin A
- Mana C
- Mangeol D
- Marchesini P
- Marian G
- Martin JP
- Marzano F
- Massaro GGG
- Mazumdar K
- McNeil RR
- Mele S
- Merola L
- Meschini M
- Metzger WJ
- Mihul A
- Milcent H
- Mirabelli G
- Mnich J
- Mohanty GB
- Molnar P
- Monteleoni B
- Moulik T
- Muanza GS
- Muheim F
- Muijs AJM
- Musy M
- Napolitano M
- Nessi-Tedaldi F
- Newman H
- Niessen T
- Nisati A
- Nowak H
- Oh YD
- Organtini G
- Ostonen R
- Palomares C
- Pandoulas D
- Paoletti S
- Paolucci P
- Paramatti R
- Park HK
- Park IH
- Pascale G
- Passaleva G
- Patricelli S
- Paul T
- Pauluzzi M
- Paus C
- Pauss F
- Peach D
- Pedace M
- Pensotti S
- Perret-Gallix D
- Petersen B
- Piccolo D
- Pierella F
- Pieri M
- Piroue PA
- Pistolesi E
- Plyaskin V
- Pohl M
- Pojidaev V
- Postema H
- Pothier J
- Produit N
- Prokofiev D
- Prokofiev DO
- Quartieri J
- Rahal-Callot G
- Rahaman MA
- Raics P
- Raja N
- Ramelli R
- Rancoita PG
- Raven G
- Razis P
- Ren D
- Rescigno M
- Reucroft S
- Riemann S
- Riles K
- Robohm A
- Rodin J
- Roe BP
- Romeo GC
- Romero L
- Rosca A
- Rosier-Lees S
- Rubio JA
- Ruschmeier D
- Rykaczewski H
- Salicio J
- Sanchez E
- Sanders MP
- Sarakinos ME
- Sarkar S
- Schafer C
- Schegelsky V
- Schmidt-Kaerst S
- Schmitz D
- Schopper H
- Schotanus DJ
- Schwering G
- Sciacca C
- Scianrino D
- Seganti A
- Servoli L
- Shevchenko S
- Shivarov N
- Shoutko V
- Shumilov E
- Shvorob A
- Siedenburg T
- Smith B
- Son D
- Spillantini P
- Steuer M
- Stickland DP
- Stone A
- Stone H
- Stoyanov B
- Straessner A
- Sudhakar K
- Sultanov G
- Sun LZ
- Suter H
- Swain JD
- Szillasi Z
- Sztaricskai T
- Tang XW
- Tauscher L
- Taylor L
- Timmermans C
- Ting SCC
- Ting SM
- Tonwar SC
- Toth J
- Tully C
- Tung KL
- Uchida Y
- Ulbricht J
- Valente E
- van Dalen JA
- van Dierendonck D
- van Gulik R
- van Rhee T
- Vesztergombi G
- Vetlitsky I
- Vicinanza D
- Viertel G
- Villa S
- Vivargent M
- Vlachos S
- Vodopianov I
- Vogel H
- Vogt H
- von der Mey M
- Vorobiev I
- Vorobyov AA
- Vorvolakos A
- Wadhwa M
- Wallraff W
- Wang M
- Wang XL
- Wang ZM
- Weber A
- Weber M
- Wienemann P
- Wilkens H
- Wu SX
- Wynhoff S
- Xia L
- Xu ZZ
- Yang BZ
- Yang CG
- Yang HJ
- Yang M
- Ye JB
- Yeh SC
- Zalite A
- Zalite Y
- Zhang ZP
- Zhu GY
- Zhu RY
- Zichichi A
- Ziegler F
- Zilizi G
- Zoller M
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/1999
- Field of study
A search for pair-produced charged Higgs bosons is performed with the L3
detector at LEP using data collected at a centre-of-mass energy of 188.6 GeV,
corresponding to an integrated luminosity of 176.4 pb^-1. Higgs decays into a
charm and a strange quark or into a tau lepton and its associated neutrino are
considered. The observed events are consistent with the expectations from
Standard Model background processes. A lower limit of 65.5 GeV on the charged
Higgs mass is derived at 95 % confidence level, independent of the decay
branching ratio Br(H^{+/-} -> tau nu)
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao W-M
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zdrazil M
- Zeitnitz C
- Zeller M
- Zema PF
- Zemla A
- Zendler C
- Zenin AV
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zilka B
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MS
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Gonzalez BA
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amram N
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- Yilmaz M
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- Zerwas D
- della Porta GZ
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
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- Zimmermann S
- Ziolkowski M
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- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fbâ1 of sâ=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan ÎČ < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
- Author
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- Abajyan T
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- Abdallah J
- Abdelalim AA
- Abdinov O
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- Yanush S
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- Yilmaz M
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- Youssef S
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- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenis T
- Zerwas D
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- Zhemchugov A
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 23/11/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal ZâČ Models
- âŠ