Search for direct top-squark pair production in final states with two leptons in pp collisions at $ \sqrt{s} $ = 8 TeV with the ATLAS detector

G Aad,A Tricoli,J Zhang,M Byszewski,A D Hawkins,J Keung,G Alexandre,V D Peshekhonov,S Patricelli,D P C Sankey,S Kohlmann,K Bos,W M Thong,P Chang,F Lanni,Y Kataoka,H Sandaker,R Sandstroem,J Brosamer,N J Cooper-Smith,H Von Der Schmitt,M C N Fiolhais,T K O Doan,R Van Der Leeuw,N Tannoury,G Mc Goldrick,M Dam,P Starovoitov,A J Lankford,Y Jiang,G Navarro,I Korolkov,E Piccaro,K K Temming,S Burdin,G Khoriauli,S I Buda,G Susinno,A Dewhurst,S Grinstein,F Rauscher,C Anastopoulos,L Alio,J L Pinfold,E Rizvi,D V Perepelitsa,I Santoyo Castillo,R Pravahan,C A Solans,M Limper,H Ten Kate,G Marchiori,V Kaushik,Q Buat,B Gibbard,T Shin,F Safai Tehrani,Yu A Tikhonov,F Rubbo,G Brown,M Backes,M Marx,O Vitells,K Amako,K J Anderson,P Grafström,P Fassnacht,J Kirk,K Mahboubi,J Elmsheuser,J Boyd,A E Kiryunin,K Nakamura,T Wenaus,B D Cooper,V Castillo Gimenez,M Petteni,A Alonso,U Bratzler,B E Cox,N Valencic,Y Cheng,F A Teischinger,R Kurumida,J Janssen,M Schwoerer,F Grancagnolo,G Zobernig,O Kind,S Pagan Griso,J Nielsen,A K Kopp,A Tykhonov,D Robinson,M Teixeira Dias Castanheira,A V Ivashin,W Wagner,J A Bogaerts,S Goldfarb,J Price,S H Kim,E Panagiotopoulou,T Dohmae,P Johansson,L Bugge,E Pueschel,A Ferretto Parodi,D T Pignotti,E Lytken,Ph Gris,A Nikiforov,J Qian,C Cuenca Almenar,F Marzano,M Ughetto,V Grassi,M Dunford,R Zitoun,P Matricon,T Koi,S Schaetzel,R Vanguri,C Deluca,F Crescioli,E Bergeaas Kuutmann,C David,G H A Viehhauser,N Morange,R Rezvani,X S Anduaga,L Gonella,K Mönig,D Lissauer,A Olszewski,L Masetti,D Prieur,S Adomeit,M Agustoni,O Arnaez,M Bomben,E Brost,B Vachon,P Gagnon,M Gouighri,P Sommer,Y Bai,M Janus,J De Graat,M P Giordani,C Mora Herrera,M Scarcella,X Zhuang,N Rompotis,B G Pope,M Wu,F Djama,V Andrei,Y B Pan,S Hamilton,R Perrino,A Di Mattia,G Arabidze,R Apolle,R L Mccarthy,S E Allwood-Spiers,S Palestini,V O’Shea,D Xu,V Chiarella,A A Snesarev,W Mohr,D Dobos,R Van Der Geer,D Lacour,F Touchard,I A Christidi,K E Varvell,D Puldon,V Rossetti,J-Y Hostachy,S Harkusha,J Donini,B Meirose,M Rose,M C Vetterli,M Flechl,G Darbo,F J Wickens,R Van Berg,D Blackburn,A C Florez Bustos,D Pohl,T Ohshima,P Tipton,C Da Via,K Belotskiy,M S Rudolph,B Kaplan,P Nevski,T A Hülsing,A Hamilton,J Cantero,A Irles Quiles,E Strauss,I Van Vulpen,S Prell,A Korn,H Torres,E Pasqualucci,L Aperio Bella,D Zanzi,Y V Grishkevich,A Ahmad,C Lapoire,A Dafinca,A Chitan,D M Gingrich,A Tua,L Serin,R Caminal Armadans,F M Newcomer,T B Sjursen,R Cherkaoui El Moursli,A Lanza,A A E Bannoura,S Youssef,L Paolozzi,A Picazio,T Mclaughlan,J Beringer,E Petrolo,K Kawagoe,C A Lee,J Cummings,A Buzatu,H Okawa,Z Hajduk,B Jackson,N Asbah,A Trzupek,P Waller,R Giordano,O Bessidskaia,P Tas,G Calderini,J A Murillo Quijada,J Walder,E Lançon,A Di Simone,F Bucci,B Dechenaux,P Berta,A Pacheco Pages,J P Thomas,G Cortiana,F Buehrer,A Gomes,Y Pylypchenko,H Ghazlane,M Nordberg,K Kordas,W-M Yao,I Wingerter-Seez,K G Tan,L Lopes,S Rosati,Z H Citron,M Fiascaris,V R Lacuesta,E Nurse,Z L Ren,N G Gutierrez Ortiz,J Ernst,I Fleck,J B Liu,J 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Asai,M Fincke-Keeler,H Fox,D Fortin,M Primavera,C Alexa,K Liu,S J Maxfield,M D Joergensen,M J Schultens,M Rammes,A Clark,D Amidei,F S Merritt,T Kondo,R De Asmundis,J Zhu,D Silverstein,S Swedish,S Laplace,M Vranjes Milosavljevic,G Mirabelli,S Williams,A Dos Anjos,R P Thun,A Di Domenico,C Schiavi,P True,T Obermann,K Gellerstedt,S Protopopescu,H L Tran,B Abi,Y Huang,L Hooft Van Huysduynen,J Cochran,U K Yang,A Succurro,M C Tamsett,A Washbrook,Y Ikegami,P Skubic,A Bellerive,D Eriksson,G D Carrillo-Montoya,E Von Toerne,S Wahrmund,H Esch,B Åsman,S Brunet,C Oropeza Barrera,J Jia,F G Sciacca,F Dittus,T Schwindt,R Ströhmer,D Wicke,K A Johns,T Lecompte,J Sjölin,E N Thompson,M Suk,F Fassi,F G Oakham,R Lafaye,Z J Grout,S Franchino,Y Okumura,H Martinez,E Shulga,B G Fulsom,R Di Sipio,A I Etienvre,D Ta,A Farbin,P Federic,L Nodulman,J Gramling,R P Middleton,G Duckeck,J Bilbao De Mendizabal,M Rescigno,A Kastanas,S Falciano,A Henrichs,E Simioni,M Shamim,F Parodi,S Maltezos,J Barreiro Guimarães Da Costa,C 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Alonso,M.-A Pleier,N Krumnack,P Dondero,F Anghinolfi,K Peters,T Harenberg,A Robson,S K Radhakrishnan,J Searcy,T Hryn’Ova,A Paramonov,M Fanti,K Desch,A Ouraou,A Knue,A Quadt,G Maccarrone,L Chen,J A Benitez Garcia,A Favareto,S Jézéquel,J Maurer,M Piccinini,K Prokofiev,R Keeler,L Chytka,J Mattmann,L Smestad,A Gorišek,I Bloch,R Rosten,I R Boyko,S Strandberg,A Ashkenazi,J Metcalfe,A Undrus,M Goblirsch-Kolb,M Biglietti,I Nikolic-Audit,M Vlasak,S W Weber,G Artoni,T Barillari,M Neumann,J Lorenz,S Kuehn,J Stark,J Weingarten,G Snidero,C Schillo,A Sansoni,G Tsipolitis,R Debbe,M A Shupe,B Heinemann,B Galhardo,K Kreutzfeldt,K Terashi,K Uchida,R Brenner,A Kuhl,C Kourkoumelis,C Gatti,N Kondrashova,L Feligioni,B Liberti,T Z Kowalski,R Wang,Y Ninomiya,S Trincaz-Duvoid,G Jones,J Howard,A White,E Etzion,Z Zhang,M Lisovyi,D Calvet,J Yu,X Wu,S Ye,A Chafaq,C Gwenlan,E Vilucchi,T Jakoubek,A V Anisenkov,J.-B Blanchard,T Colombo,T Guillemin,R Nicolaidou,R Mount,S S A Livermore,T Varol,E Schmidt,P Rieck,E Shabalina,A T Law,K Mochizuki,E Ladygin,A Nisati,R A Mcpherson,K Kiuchi,P Laycock,B Weinert,V V Sulin,S Tokár,A Campoverde,G G Hesketh,F Bauer,M Fraternali,G Lefebvre,Y Suzuki,S Leontsinis,F Corriveau,M P Casado,K Yamamoto,C Meroni,D Rousseau,V Nikolaenko,G Amundsen,T Serre,C Santoni,F Spanò,V Garonne,F Zhang,G Galster,A I Mincer,R Leone,C Giuliani,F Monticelli,D Hoffmann,S M Farrington,S Meehan

doi:10.1007/jhep06(2014)124

Abstract

A search is presented for direct top-squark pair production in final states with two leptons (electrons or muons) of opposite charge using 20.3fb-1 of pp collision data at sqrt(s)=8TeV, collected by the ATLAS experiment at the Large Hadron Collider in 2012. No excess over the Standard Model expectation is found. The results are interpreted under the separate assumptions (i) that the top squark decays to a b-quark in addition to an on-shell chargino whose decay occurs via a real or virtual W boson, or (ii) that the top squark decays to a t-quark and the lightest neutralino. A top squark with a mass between 150 GeV and 445 GeV decaying to a b-quark and an on-shell chargino is excluded at 95% confidence level for a top squark mass equal to the chargino mass plus 10 GeV, in the case of a 1 GeV lightest neutralino. Top squarks with masses between 215 (90) GeV and 530 (170) GeV decaying to an on-shell (off-shell) t-quark and a neutralino are excluded at 95% confidence level for a 1 GeV neutralino.

Highlights

Background fitThe observed numbers of events in the control regions (CRs) are used to derive SM background estimates in each signal regions (SRs) via a profile likelihood fit [89]
A top squark with a mass between 150 GeV and 445 GeV decaying to a b-quark and an on-shell chargino is excluded at 95% confidence level for a top squark mass equal to the chargino mass plus 10 GeV, in the case of a 1 GeV lightest neutralino
For the case of a 1 GeV neutralino, a top-squark t1 with a mass between 150 GeV and 445 GeV decaying to a b-quark and a chargino is excluded at 95% confidence level (CL) for a chargino approximately degenerate with the top squark

Summary

The ATLAS detector

The detector layout consists of inner tracking devices surrounded by a superconducting solenoid, electromagnetic and hadronic calorimeters and a muon spectrometer. The ID is surrounded by a thin superconducting solenoid providing a 2T axial magnetic field and it provides precision tracking of charged particles and vertex reconstruction. The calorimeter system covers the pseudorapidity range |η| < 4.9. In the region |η| < 3.2, high-granularity liquid-argon electromagnetic. The end-cap and forward regions, which cover the range 1.5 < |η| < 4.9, are instrumented with liquid-argon calorimeters for both electromagnetic and hadronic particles. The muon spectrometer surrounds the calorimeters and consists of three large superconducting air-core toroid magnets, each with eight coils, a system of precision tracking chambers (|η| < 2.7) and fast trigger chambers (|η| < 2.4)

Monte Carlo simulations and data samples

Physics object selection

Preselection and event variables

Leptonic mT2 selection

Hadronic mT2 selection

Multivariate analysis

Standard Model background determination

Background fit

Fake and non-prompt lepton background estimation

Leptonic mT2 analysis

Hadronic mT2 analysis

Systematic uncertainties

Background

Results and interpretation

Conclusions

A Generator-level object and event selection

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Journal: Journal of High Energy Physics	Publication Date: Jun 1, 2014
Citations: 115	License type: cc-by

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Search for direct top-squark pair production in final states with two leptons in pp collisions at $ \sqrt{s} $ = 8 TeV with the ATLAS detector

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Search for direct top-squark pair production in final states with two leptons in pp collisions at $ \sqrt{s} $ = 8 TeV with the ATLAS detector

Abstract

Highlights

Summary

Talk to us

Similar Papers

More From: Journal of High Energy Physics