Search for Dilepton Resonances inppCollisions ats=7  TeVwith the ATLAS Detector

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Wittgen,X Zhang,N F Castro,E Perez Codina,P Calafiura,M Mathes,K Shaw,H Von Der Schmitt,A Barbaro Galtieri,A Mengarelli,C Santoni,P A Delsart,D Tsybychev,J L Lane,E Ladygin,R Ishmukhametov,T P A Åkesson,C Grah,L S Ancu,S Jakobsen,L Mijović,S V Morozov,T Dai,H Matsumoto,D Sherman,B Butler,T Stockmanns,V Izzo,Ph Martin,G Blanchot,M Rijpstra,R Di Sipio,L Nicolas,L P Says,A Boveia,M Ibbotson,E Magradze,M Mikuž,P Vankov,M W Wolter,E Brodet,T Zhao,T Eifert,E Van Der Poel,P Pralavorio,T Bain,A Sidoti,N Makovec,A Manz,M Morii,T Alexopoulos,J L Schlereth,H Guler,U Husemann,Y Fang,C Schwanenberger,M Ernst,A Salamon,E Vilucchi,C.-M Cuciuc,A C Martyniuk,R W Moore,R B Nickerson,V Vorwerk,P Krieger,K Kawagoe,D Kar,T Naumann,M Weber,Y Pylypchenko,A Bertin,B Vachon,B P Kerševan,M Cobal,M Zeller,N A Mccubbin,Y V Grishkevich,M Petteni,R Mandrysch,F Hubaut,C G Lester,A D Doxiadis,M Campanelli,F J Tique Aires Viegas,H O Danielsson,D Tsionou,Y Tanaka,Y Azuma,F S Merritt,C Suhr,A E Kiryunin,L Sawyer,M Idzik,V Kukhtin,S Xie,P F Giraud,J Z Will,S Yanush,D R Tovey,F Winklmeier,P Laycock,J Lesser,W Davey,C Bernius,D H Saxon,P Buchholz,X Espinal Curull,M Fehling-Kaschek,J Odier,P A Love,M Donegà ,S C Zenz ,T Löhse ,P Némethy ,M Marčišovský ,M Bóna ,G Schüler ,H J Yang ,C Santamarina Ríos ,D Tureček ,J M Cook ,Vladimiro Tikhomirov ,B Selldén ,L P Calôba ,R Kass ,A A Salnikov ,E Le Ménédeu ,V Král ,T Mäshimo ,Alexei Talyshev ,Z Hubáček ,S González ,Yoshihiro Suzuki ,P Conde Muíño ,S Thomä ,Marcos Vinicius Silva Oliveira ,M S Soares ,S A Çetin ,L Hervás ,J Krstić ,Z Drásal ,S Němeček ,L L ,Yu M Sviridov ,M Fisher ,V Lombardo ,P Vokáč ,J Šolc ,E Castaneda‐Miranda ,G Ünel ,E Banaś ,F Muêller ,T Pérez Cavalcanti ,J S.h Lee ,A Ruiz-Martínez ,R Miller ,Roger Jones ,P Řezníček ,И Орлов ,N Öztürk ,Philippe Ghez ,J Pína ,M Taševský ,T Akdoğan ,W Dąbrowski ,J Hřivnáč ,A G Bogdanchikov ,J Kapłon ,J Labbé ,M L Andrieux ,P Kodyš ,F Henry‐Couannier ,V E Özcan ,T Bołd ,K Jon‐And ,J Jakůbek ,A Kupčo ,J Günther ,A Maŕın ,P V.m Da Silva ,M Goêbel ,J Colás ,M Villaplana Pérez ,O Jönsson ,H.‐C Schultz‐Coulon ,E Richter-Wąs ,A Léger ,D Salihagić ,J P Martín ,R Mäenner ,I Vukotić ,E Górnicki ,J Chapman ,N D Patel ,G Otero Y Garzón ,Feng Tian ,M Martínez ,T Slavíček ,Z Doležal ,Lj Simić ,D Strom ,A M Soukharev ,D Kollár ,Jean-Christophe Gayde ,D Hayden ,I Borjanović ,J Błocki ,A Randle-Conde ,L Kirsch ,В А Гапиенко ,S.‐C Hsu ,J Dolejší ,Š Todorova-Nová ,M Myška ,M Karagöz ,Peter Steinbach ,P Y Nechaeva ,O M Kind ,L A.m Wiik ,M Arık ,D Bànfi ,P Stríženec ,A K Çiftçi ,Satoshi Tanaka ,A Robichaud-Véronneau ,F Köhn ,Takashi Sasaki ,Ö Runólfsson ,M Smižanská ,C Garćıa ,A A Korol ,N Vranješ ,J Muêller ,A Bingül ,А Антонов ,B Rückert ,T P Kokott ,S Diţă ,M A Pleier ,T Holý ,A Llères ,E Arık ,A Gutiérrez ,S Moêd ,B Demirköz ,S Martin–Haugh ,Han Liu ,S Iştin ,S González-Sevilla ,K Jeleń ,T Kühl ,A Žsenei ,L Nožka ,T Sloan ,S Banerjee ,M Mikeštíková ,P Diţâ ,H S Subramania ,W Iwański ,M A Dufour ,J Idárraga ,I Grabowska-Bołd ,M Svatoš ,J K Kraus ,M Dwužnik ,Michael Price ,D Ziemińska ,И И Цукерман ,M Yılmaz ,J Linnemann ,В Н Гущин ,I Türk Cakir ,T Sýkora ,S Bürke ,F Ë Taylor ,B Mansoulié ,Yuan Li ,P Gutiérrez ,Benedict Martin Waugh ,Н Григалашвили ,B Lund‐Jensen ,D Bretón ,V Juránek ,A Jérémie ,À Zoccoli ,R Plačakytė ,Ç İşsever ,D Kühn ,C Böhm ,R Brunelière ,C Bélanger-Champagne ,M Houlden ,V L Malyshev ,C Royon ,T Blažek ,J Schovancová ,M P Kelly ,J Tóth ,S Henrot-Versillé ,П Б Шаталов ,R Çiftçi ,C C Young ,J De Vivie De B Regie ,M A Díaz ,I Božović-Jelisavc̆ić ,V.a Kazanin ,A Castaneda Hernandez ,Akira Shibata ,D S Popović ,S Dubé ,I Mandić ,A Filipčǐc ,V A Giakoumopoulou ,O Çakır ,Yu A Tikhonov ,J R Lessard ,И Н Александров ,B Clément ,A.a Grillo ,Š Valkár ,E Reinherz‐Aronis ,E Lançon ,C Schröeder ,L Skinnari ,J Nováková ,M Cavalli‐Sforza ,I Sýkora ,M Ziółkowski ,C Clément ,D Rodriguez Rodriguez ,S Cŕéṕe-Renaudin ,M Turała ,В Г Бондаренко ,N Semprini‐Cesari ,A E Nuncio-Quiroz ,J Große-Knetter ,M L Kocian ,Th Müller ,E Yu Soldatov ,G Brandenburg ,Y Zalite ,Matthew Henry Klein ,T Ekelöf ,J Antos̆ ,T Davídek ,G Lütz ,C Gößling ,Hiroshi Takeda ,J L Ping ,T Horažďovský ,I Eschrich ,V Šimák ,C Stănescu ,M Lokajı́ček ,E Rulikowska-Zarȩbska ,S Pospı́šil ,J Mašík ,V I Ruď ,D Reljić ,Y Pan ,M V Purohit ,Dj Šijački ,P Šı́cho ,J Terrón ,A Dʼorazio ,В А Коротков ,P Kadlečík ,J.c-L Tseng ,A Martín ,A Hidvégi ,А Хорошилов ,G Pásżtor ,P Růžička ,Martin Weber ,M Havránek ,S Martí-García ,Г Атоян ,C Timmermans ,E Augé ,D Ferrère ,I Štekl ,F Quiñónez ,J Braciník ,Yi Yang

doi:10.1103/physrevlett.107.272002

Abstract

This Letter reports on a search for narrow high-mass resonances decaying into dilepton final states. The data were recorded by the ATLAS experiment in pp collisions at sqrt(s) = 7 TeV at the LHC and correspond to a total integrated luminosity of 1.08/fb (1.21/fb) in the ee (mumu) channel. No statistically significant excess above the Standard Model expectation is observed and upper limits are set at the 95% C.L. on the cross section times branching ratio of Z' resonances and Randall-Sundrum gravitons decaying into dileptons as a function of the resonance mass. A lower mass limit of 1.83 TeV on the Sequential Standard Model Z' boson is set. A Randall-Sundrum graviton with coupling k/M_Pl=0.1 is excluded at 95% C.L. for masses below 1.63 TeV.

Highlights

DimuonsNormalization parton distribution functions (PDFs)= S QCD K factor Weak K factor Trigger/reconstruction Total5% Not applicable Not applicable Not applicable Negligible 5%week ending 30 DECEMBER 2011 diboson and W þ jets backgrounds from Monte Carlo simulation are scaled according to their respective cross sections and added to the QCD background
The scaling factor is within 1% of unity
The advantage of this approach is that the uncertainty on the luminosity

Summary

85 Æ 5 150 Æ 26 191 Æ 75 6128 Æ 200

The Z= Ã cross section is calculated at next-to-next-toleading order (NNLO) using PHOZPR [36] with MSTW2008 PDFs [37]. The ratio of this cross section to the leadingorder cross section is used to determine a mass-dependent QCD K factor which is applied to the results of the leadingorder simulations. In the reversed electron identification technique, data with both electron candidates failing some identification criteria (chosen not to affect kinematic distributions) are used to determine the QCD background distribution versus mee This method is used for the central estimate and the others which bracket it, to assign a systematic uncertainty.

Background

Z0 models