Measurements of the top quark branching ratios into channels with leptons and quarks with the ATLAS detector

G Aad,S Kreiss,M Vranjes Milosavljevic,H Von Der Schmitt,B Lopez Paredes,O Simard,I Chalupkova,E Romero Adam,J Del Peso,P Lichard,R Camacho Toro,S Gadomski,A Ezhilov,Pa Malecki,X Hu,B Stugu,G Polesello,N Van Eldik,E Valladolid Gallego,R Cherkaoui El Moursli,A Palma,G Akimoto,V Boldea,A Glazov,V Chernyatin,E Von Toerne,M Franklin,D Su,S Cabrera Urbán,S Argyropoulos,J Zhong,I Massa,R Mandrysch,D Guest,J-Y Hostachy,D Macina,A Salamon,L Lambourne,J Proudfoot,M Morii,L Feremenga,T Scanlon,Z Vykydal,D Ventura,S Willocq,Y Munwes,K Ntekas,M Uhlenbrock,G Gonzalez Parra,T Bain,R Kowalewski,G Carlino,M Wittgen,C Tsarouchas,A Ferretto Parodi,W Kozanecki,M Sosebee,J Nadal,E Hines,S Schaetzel,Y Bai,E Sedykh,A De Salvo,C Suhr,B Auerbach,C Oropeza Barrera,J Silva,A Kobayashi,S Pagan Griso,P Chang,D Pohl,H Kagan,R Sandstroem,A Pranko,L De Nooij,M Beretta,F Marzano,E Musto,B Gaur,W Mohr,A Di Ciaccio,E Strauss,H Namasivayam,G Anders,T Dohmae,C Hengler,M Losada,M Marx,M Crispin Ortuzar,C Conta,V Andrei,A Altheimer,V Consorti,F De Lorenzi,F Lasagni Manghi,A Kapliy,A Henrichs,J Wetter,K Amako,K Nakamura,R De Asmundis,R Herrberg-Schubert,P Skubic,T Kobayashi,N Soni,N De Groot,T Cuhadar Donszelmann,H Pirumov,Y Li,R Simoniello,H Ghazlane,F Salvatore,W Bhimji,G Nunes Hanninger,Y Silver,J Wotschack,M Kaci,D Di Valentino,S Prell,L Zanello,D Lissauer,Y Davygora,M Warsinsky,N Tannoury,M Kuze,A Ferrer,R Caminal Armadans,O Le Dortz,M Abolins,A Loginov,P Loscutoff,M Cano Bret,S Viel,I Van Vulpen,A Bruni,T Todorov,L La Rotonda,J Griffiths,E Jansen,D Levin,R Subramaniam,M Trottier-Mcdonald,J Tanaka,E Le Guirriec,C Bacci,S Jin,K Tollefson,T Spreitzer,H Van Der Graaf,Ph Schune,C Cuthbert,L Bugge,S Errede,D Paredes Hernandez,L Hooft Van Huysduynen,Y Jiang,P Van Gemmeren,M Faucci Giannelli,P True,Y Benhammou,N Lorenzo Martinez,M Pedersen,M Battaglia,A Andreazza,S Nektarijevic,D Jennens,T Hayashi,E Ptacek,P Gauzzi,B Sarrazin,P Johansson,C Pizio,D Hellmich,J Stahlman,J Schwindling,M Kaneda,C Deluca,Y 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,Y Liu,C Fukunaga,P D Thompson ,P Kodyš ,S P Ahlen ,A Saddique,J Carvalho,J A Frost ,J A Benitez Garcia ,Y Yamaguchi,N Nikiforou,D A A Geerts ,F G Oakham ,C Bini,K Kawagoe,B Yabsley,H Oide,L March,E Petrolo,S C Lin ,J Guo,R Gonçalo,A Tykhonov,S W Weber ,D Scheirich,C Serfon,I Sýkora ,T P S Gillam ,H Severini,M Vreeswijk,N R Bernard ,X Wu,R Cardarelli,A Poppleton,J Adelman,L J Beemster ,S Raddum,P L Rosendahl ,G N Taylor ,C Taccini,E Mountricha,G Qin,J Zhang,D Hayden,S Cheatham,J Schovancová ,J A Bogaerts ,E Pasqualucci,K Prokofiev,J Jovicevic,M Livan,S Hageböck,O Çakır ,C Deterre,L L ,E Cheremushkina,O L Rezanova ,J Cochran,M Neumann,C Troncon,K Kroeninger,A Chitan,D Pelikan,T Koi,G Poulard,R Nicolaidou,R Polifka,T Klioutchnikova,F O’Grady,D K Jana ,D O Jamin ,A T Watson ,Y Coadou,J M Iturbe Ponce ,C A Solans ,M Ishino,K Desch,R Stroynowski,A Kotwal,J E Derkaoui ,K K Temming ,E Lançon,À Zoccoli ,A Strandlie,M Queitsch-Maitland,J M Butler ,H M Gray ,S Vlachos,D S Popović ,А Антонов ,J 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Semprini‐Cesari ,B Osculati,I López Paz ,M Kuna,M Rotaru,S Hasegawa,R Hickling,R B Nickerson ,F Ould-Saada,L Serin,P Urquijo,J Krstić ,H M X Grabas ,P J Lösel ,T Naumann,Y Zhao,T J Neep ,G A Stewart ,A Baroncelli,O Ricken,N Flaschel,S Diglio,A Nelson,S Hou,G Navarro,V Jain,I Brock,O Brandt,P Stolte,J P Grohs ,F G Sciacca ,A R Weidberg ,U Bratzler,F Hoenig,D L Adams ,A Chegwidden,S Constantinescu,D T Pignotti ,F Lanni,M Donadelli,R W Gardner ,E Etzion,A Mehta,P Fassnacht,S Turchikhin,M Homann,A Maevskiy,T Barklow,O V Solovyanov ,S Oda,M J Tibbetts ,N Berger,P Urrejola,H Torres,C Malone,S Richter,Y Smirnov,J Cantero,V Chiarella,M W Krasny ,J Godlewski,G Salamanna,M Sessa,M Spousta,Seyed Ruhollah Shojaii ,C Schillo,S Asai,M Schumacher,F M Garay Walls ,N Huseynov,G Redlinger,M Smižanská ,M Spalla,Y Yasu,E Stanecka,K Köneke,L Mapelli,B Gorini,O Kivernyk,G H A Viehhauser ,S Kluth,M Lévy ,R Zhang,S Gadatsch,S J Head ,S Tsiskaridze,S P Marsden ,H Ogren,J Wakabayashi,T Javůrek,M Costa ,M K Ayoub ,D M Gingrich ,K Augsten,P A Bruckman De Renstrom ,R Mount,J Schaarschmidt,I Korolkov,M Weber ,A Ovcharova,X Zhuang,K Chen,M Fanti,D C O’neil ,R Schwienhorst,P R Newman ,S Lammers,C Sbarra,D Sidorov,J Mahlstedt,K Ikematsu,F Fiedler,A D Pilkington ,K J Anderson ,K Cranmer,S A Olivares Pino ,A Washbrook,A Coccaro,D P Benjamin ,J E Sundermann ,J Wittkowski,J Meyer,N Kondrashova,J Erdmann,E Carquín ,J P Rutherfoord ,J J Chwastowski ,D Boumediene,E A Ouellette ,M Scarcella,M Testa,C Gwenlan,Yuan Li ,P Calafiura,M Corradi,O Zenin,K Hamano,M Sławińska ,H Arnold,R Leone,R D Mudd ,K Sapp,P J Hsu ,K Černý ,J Penwell,F M Brochu ,K Motohashi,F Ceradini,J Olszowska,A Zhemchugov,N P Dang ,D Whiteson,L F Marti ,C Sandoval,A Lister,J Jentzsch,Z V Krumshteyn ,S L Barnes ,J Howard,Dj Šijački ,J Mašík ,H F-W Sadrozinski ,W B Quayle ,F Kiss ,C Gabaldon,P Giannetti,M Becker,F Pastore,M Aoki,Steffen Staerz ,C Wanotayaroj,P Steinberg,J D Chapman ,J Yu,M Owen,D Nguyen ,L Alio,S Wahrmund,E Ros,M 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Li,C M Hawkes ,M Svatoš ,E Simioni,B Giacobbe,M Bosman,R A Mcpherson ,A J Bevan ,B Lund‐Jensen ,A R Buzykaev ,N Garelli,S Molander,M Ughetto,B Weinert,H Öhman ,N A Mccubbin ,M T Pérez García-Estañ ,T Kondo,E Lobodzinska,J R Catmore ,J Rieger,Κ Παπαγεωργίου ,F Bauer,V Cindro,D Madaffari,P Diţâ ,P Conde Muíño ,I Vichou,S Tapprogge,S I Buda ,H Oberlack,M Thomson,P Sommer,A A Talyshev ,M J Flowerdew ,K Krizka,N C Edwards ,R Vari,P F Harrison ,K Wang,T B Sjursen ,E Gorini,F J Wickens ,M R Jaekel ,P F Giraud ,H Iwasaki,L Y Shan ,C M Delitzsch ,T Golling,E J W Moyse ,F Muêller ,D Emeliyanov,L Jeanty,A Kugel,C Bernard,S Camarda,C Petridou,N Öztürk ,J E M Robinson ,M Solar,R Vanguri,C P Ward ,H Lacker,Thomas Schwarz ,M Talby,A Cortes-Gonzalez,C F Anders ,N Taiblum,W Wiedenmann,R Voss,M Slater,H Chen,T B Huffman ,M C Hodgkinson ,V A Kantserov ,З Маршалл ,T A Martin ,Y Nagai,M Saleem,P Schacht,A Dattagupta,Z Barnovska,K Yoshihara,J B Liu ,L Brenner,P Bechtle,E Coniavitis,M Fincke-Keeler,R Abreu,L Beresford,N Zhou,M Begel,F Bertolucci,H K Hadavand ,V P Maleev ,L A M Wiik-Fuchs ,L Heinrich,M W Wolter ,Z M Karpova ,C Hsu,R Staszewski,T Vazquez Schroeder,M Düren,M Ernst,S Watts,B Axen,P K Teng ,J Alison,C Escobar,J Janssen,V Bortolotto,A Ruiz-Martínez ,K Sekhon,R Debbe,G Mornacchi,P Gallus,E Gozani,P Kluit,S Hassani,M Hirose,S Binet,A J Beddall ,V O Tikhomirov ,R Thun ,A Rimoldi,Y Horii,B E Cox ,D Lynn,P P Allport ,H M Braun ,G Azuelos,F Prokoshin,M P Giordani ,V A Kramarenko ,N Rompotis,C Clément ,F Ragusa,I Bloch,Y S Gao ,N Andari,G H Herbert ,V Vacek,J Howarth,S P Denisov ,P Bagnaia,A Fischer,F Corriveau,S Falciano,A E Baas ,C Leroy,T Blažek ,M Janus,A G Kharlamov ,P Savard,E Richter-Wąs ,O M Kind ,C Weiser,D A Maximov ,M Atkinson,K Grimm,S Sun,G J Bobbink ,A Wildauer,P Rieck,T Ekelöf ,K Hamacher,S Pedraza Lopez,M Červ ,P J Clark ,D A Scannicchio ,N Orlando,M K Bugge ,Z Zinonos,S Terzo,K Bendtz,A Oh,A Tavares Delgado,H J Lubatti ,K Shaw,R N Clarke ,F Ukegawa,S Angelidakis,A Soffer,D Strom ,M I Gostkin ,A Sanchez,D Bullock,H Santos,X Ruan,G Herten,J Monk,C Bock,E Paganis,S M Romano Saez ,Y Yamazaki,J G Panduro Vazquez ,E V Bouhova-Thacker ,A Alonso,C Amelung,M C N Fiolhais ,A Tricoli,A K Çiftçi ,R Brunelière ,S Schramm,P A Love ,R M Fakhrutdinov ,C Santoni,T Wang,E Shabalina,W R Spearman ,J E Black

doi:10.1103/physrevd.92.072005

Abstract

Measurements of the branching ratios of top quark decays into leptons and jets using events with $t \overline{t}$ (top antitop) pairs are reported. Events were recorded with the ATLAS detector at the LHC in pp collisions at a center-of-mass energy of 7 TeV. The collected data sample corresponds to an integrated luminosity of 4.6 ${\mathrm{fb}}^{-1}$. The measured top quark branching ratios agree with the Standard Model predictions within the measurement uncertainties of a few percent.

Highlights

In the Standard Model (SM), 100% of the top quark decays contain a W boson and a down-type quark
In the SM the branching ratio to the different leptons is the same since the decay proceeds via a W boson, but in models of new physics, e.g. supersymmetry (SUSY), final states with τ leptons can be enhanced or suppressed [5]; measuring the inclusive cross section using final states with τ leptons can be a good probe for new physics
The measured values of the top quark branching ratios will deviate with respect to the SM predictions if the data sample selected to extract tt events contains final states without two W bosons

Summary

INTRODUCTION

In the Standard Model (SM), 100% of the top quark decays contain a W boson and a down-type quark. Limits on the top quark branching ratio to a charged Higgs boson and a b-quark have been published by the CDF [6], D0 [7,8], ATLAS [9,10] and CMS [11] collaborations Another example of a final state that can change the observed branching ratios is the pair production of supersymmetric partners of the top quark (~t) decaying into bνττ~ followed by the τ~ decay into a τ lepton and the gravitino, predicted by gauge-mediated SUSY breaking models [12]. Branching ratios for semileptonic and purely hadronic top quark decays are obtained by combining these seven final states assuming that only SM processes contribute to the background and the top branching ratios to leptons and jets add up to one

ANALYSIS OVERVIEW

ATLAS DETECTOR

DATA AND MONTE CARLO SAMPLES

EVENT SELECTION

SINGLE-LEPTON þ JETS CHANNEL

Background templates

Fits to mass distributions

DILEPTON þ JETS CHANNEL

VIII. LEPTON þ τhad þ JETS CHANNEL

Tau background templates

Signal extraction by fitting to BDTj shape

17 Æ 8 442 Æ 15 1440 Æ 40

Fit results

MEASURING CROSS SECTION AND BRANCHING RATIOS

SYSTEMATIC UNCERTAINTIES

RESULTS

CONCLUSION

Methods

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Journal: Physical review. D, Particles and fields	Publication Date: Oct 19, 2015
Citations: 10	License type: CC BY 3.0

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Measurements of the top quark branching ratios into channels with leptons and quarks with the ATLAS detector

Abstract

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Measurements of the top quark branching ratios into channels with leptons and quarks with the ATLAS detector

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