Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at sqrt{s}=13 TeV

A A Bin Anuar,A Baden,A Bat,A Bodek,A Bornheim,A C König ,A Calderón ,A Canepa,A Carvalho Antunes De Oliveira,A Castaneda Hernandez,A David,A De Cosa,A De Roeck,A De Wit,A Delgado Peris,A Di Francesco,A Di Mattia,A Escalante Del Valle,A G Stahl Leiton,A García-Bellido ,A Kayis Topaksu,A Lopez Virto,A Melo,A Meyer,A Morelos Pineda,A Quintario Olmeda,A Ranieri,A Richards,A Rinkevičius ,A Rizzi,A Rose,A Rácz ,A Rýd ,A Sánchez-Hernández ,A Vilela Pereira,A Vorobyev,A Çakır ,A Çelik ,Adeel Ahmad ,Alberto Orso Maria Iorio ,Andrew Johnson ,Antônio Rossi ,Arun Kumar,Ashok Kumar,Ashraf Mohamed ,B Akgün ,B Chazin Quero,B De La Cruz,B E Cox ,B Jayatilaka,B Tali,B Ujvári ,B Wysłouch ,C A Carrillo Montoya,C Barth,C Diez Pardos,C F Gonźalez Herńandez ,C Fernandez Bedoya,C Hajdú ,C Martínez Rivero ,C Mesropian,C Mora Herrera,C Neu,C Oropeza Barrera,C Peng ,C Peña ,C S Moon,C Scharf,C Tuvé ,C Uribe Estrada,C Vander Velde,C Wissing,C Ávila ,Chia‐Ming Kuo ,D A Sanz Becerra,D Blöch ,D De Jesus Damião ,D Del Re,D Di Croce,D Ferenček ,D Horváth ,D Kotliński ,D R Claes,D Sunar Cerci,D Ćutts ,Deepak Kumar Sahoo ,E A De Wolf,E Belchior Batista Das Chagas,E Carrera Jarrin,E Clément ,E Currás ,E De La Cruz-Burelo,E Di Marco,E Eskandari Tadavani,E J Tonelli Manganote,E M Da Costa,E Palencia Cortezon,E Pérez ,E Torassa,E W Hughes ,E W Vaandering,F De Guio,F Gasparini,F M Stober,F Nessi‐Tedaldi ,F Pauß ,F Rezaei Hosseinabadi,F Siklér ,F Simonetto,F Torres Da Silva De Araujo,F Vazquez Valencia,F Özok ,Faridah Mohamad Idris ,Feng Liu ,G B Mohanty,G B Yu,G De Lentdecker,G Della Ricca,G G Da Silveira,G Gomez Ceballos,G Grenier,G Gómez ,G Gökbulut ,G L Pinna Angioni,G M Bilei,G M Dallavalle,G Martı́nez ,G Mäggi ,G N Kim,G P Siroli,G P Van Onsem,G Pásżtor ,G Zevi Della Porta,G Önengüt ,Gian Michele Innocenti ,H A Salazar Ibarguen,H Białkowska ,H Castilla‐Valdez ,H El Mamouni,H Flächer ,H Lee,H Oğul ,H S Chen,H Van Haevermaet,H W Wulsin,H Wei,Hannsjoerg Artur Weber ,I D Sandoval Gonzalez,I De Bruyn,I 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doi:10.1007/jhep06(2018)027

Abstract

A search for dark matter is conducted in events with large missing transverse momentum and a hadronically decaying, Lorentz-boosted top quark. This study is performed using proton-proton collisions at a center-of-mass energy of 13 TeV, in data recorded by the CMS detector in 2016 at the LHC, corresponding to an integrated luminosity of 36 fb−1. New substructure techniques, including the novel use of energy correlation functions, are utilized to identify the decay products of the top quark. With no significant deviations observed from predictions of the standard model, limits are placed on the production of new heavy bosons coupling to dark matter particles. For a scenario with purely vector-like or purely axial-vector-like flavor changing neutral currents, mediator masses between 0.20 and 1.75 TeV are excluded at 95% confidence level, given a sufficiently small dark matter mass. Scalar resonances decaying into a top quark and a dark matter fermion are excluded for masses below 3.4 TeV, assuming a dark matter mass of 100 GeV.

Highlights

Hadronically decaying top quark identificationIf a hadronically decaying top quark is highly Lorentz-boosted, reconstructing the three daughter quarks separately becomes difficult, as the resulting jets tend to overlap in the detector
Expected and observed limits at 95% confidence level (CL) are set using the asymptotic approximation [57] of the CLs criterion [58, 59] with a profile likelihood ratio as the test statistic, in which systematic uncertainties are modeled as nuisance parameters
To allow for reinterpretation of the data in the context of signal models not considered in this paper, we provide the results of fitting data in the control regions (CR) and propagating the prediction to the signal region (SR) in appendix A

Summary

Hadronically decaying top quark identification

If a hadronically decaying top quark is highly Lorentz-boosted, reconstructing the three daughter quarks separately becomes difficult, as the resulting jets tend to overlap in the detector To identify such signatures, we define CA15 jets as objects that are clustered from PF candidates using the Cambridge-Aachen algorithm [30] with a distance parameter of 1.5. The “soft drop” (SD) [33] grooming method is used to remove soft and wide-angle radiation produced within jets through initial state radiation or through the underlying event Removing such radiation, the SD algorithm defines a subset of the CA15 jet’s constituents, which are further grouped into subjets of the CA15 jet. The chosen threshold corresponds to correctly identifying a bottom jet with a probability of 80%, and misidentifying a light-flavor jet with a probability of 10%

Substructure

Signal topology selection

Background rejection

Signal estimation

Control regions

Transfer factors

Systematic uncertainties

Results

Summary

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Journal: Journal of High Energy Physics	Publication Date: Jun 1, 2018
Citations: 24	License type: open-access

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Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at sqrt{s}=13 TeV

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Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at sqrt{s}=13 TeV

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