Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at sqrt{s}=13 TeV

A A Bin Anuar,A Bat,A Bodek,A Bornheim,A Bragagnolo,A Calderón ,A Delgado Peris,A Di Mattia,A Escalante Del Valle,A García-Bellido ,A Rácz ,A Rýd ,A Sánchez-Hernández ,A Vagnerini,A Vilela Pereira,A Çakır ,A Çelik ,Alberto Orso Maria Iorio ,Andrey Popov ,Anne-Laure Pequegnot ,Arun Kumar,Ashok Kumar,B Akgün ,B Chazin Quero,B Işıldak ,B Mcmaster,B Tali,B Ujvári ,B Wysłouch ,Benjamin Charles Radburn-Smith ,C Diez Pardos,C F Gonźalez Herńandez ,C Fernandez Bedoya,C Hajdú ,C Martínez Rivero ,C Schwanenberger,C Tuvé ,C Vander Velde,C Ávila ,Chia‐Ming Kuo ,Clemencia Mora Herrera ,D Blöch ,D De Jesus Damiao,D Di Croce,D Doḿınguez Damiani ,D Ferenček ,D Horváth ,D Kotliński ,D Soldi,D Ćutts ,Dan Yu ,Daniel John Karmgard ,David Romero Abad ,Diego Matos Figueiredo ,E Carrera Jarrin,E Clément ,E De La Cruz-Burelo,E Di Marco,E Eskandari Tadavani,E Palencia Cortezon,E Pérez ,Eric Christian Chabert ,F Canelli ,F Nessi‐Tedaldi ,F Pauß ,F Rezaei Hosseinabadi,F Siklér ,F Simonetto,F Vazzoler,F Özok ,Feng Liu ,Fábio Lúcio Alves ,G Bauer,G Cucciati,G De Lentdecker,G Della Ricca,G G Da Silveira,G Gómez ,G Gökbulut ,G Hamel De Monchenault ,G Martı́nez ,G Mäggi ,G P Siroli,G P Van Onsem,G Paspalaki,G Pásżtor ,G Zevi Della Porta,G Önengüt ,Gian Luca Pinna Angioni ,Gian Michele Innocenti ,Guillelmo Gomez Ceballos ,H Białkowska ,H Castilla‐Valdez ,H El Mamouni,H Flächer ,H Oğul ,H S Chen,H Sert,Hannsjoerg Artur Weber ,Hans-Christian Kaestli ,Humberto Antonio Salazar Ibarguen ,I Babounikau,I De Bruyn,I Dumanoğlu ,I González Caballero ,I Hoş ,I Van Parijs,Imad Baptiste Laktineh ,J Alcaraz Maestre,J Andreä ,J D Tapia ∋Takaki ,J Fernández Menéndez ,J Hoß ,J Królikowski ,J Königsberg ,J L Dulemba,J M Hernández ,J Malclès ,J Milošević ,J Molnár ,J Piedra Gomez,J R Gonźalez Ferńandez ,J W Gary,Jaehoon Lim ,James John Brooke ,Jesús Puerta Pelayo ,Joern Schwandt ,Jui-Fa Tsai ,K Buńkowski ,K Cankoçak ,K Ehataht,K Hurtado Anampa,K Höepfner ,K M Ecklünd ,K Vellidis,K Wichmann,K Özdemir ,Kristan Allan Hahn ,L Alunni Solestizi,L Brigliadori,L Felď ,L Lloret Iglesias,M Besançon ,M Calderón De La Barca Sánchez ,M Csanád ,M De Mattia,M Della Negra,M Déjardin ,M Fernández ,M Flechl,M Grünewald ,M Kröhn ,M Lipiński ,M M Defranchis,M Melo De Almeida,M Mohammadi Najafabadi,M Schmitt ,M Van De Klundert,M Vander Donckt,M Vidal Marono,Maksym Titov ,Mara Senghi Soares ,Mauro Emanuele Dinardo ,Merve Nazlım Ağaras ,Michael Benjamin Andrews ,Mirena Ivova Paneva ,Mohd Adli Bin Ali ,N Béni ,N De Filippis,N Filipović ,N Godinović ,N Van Remortel,O Buchmüller ,O González López ,O Hlushchenko,O Kukral,O Long ,O Rieger,P Adžić ,P Das,P Kontaxakis,P Maksimović ,P Martínez Ruiz Del Arbol ,P Milenović ,P Priyanka,P Rebello Teles,P Van Hove,P Van Mechelen,P Van Mulders,P De Barbaro,Peter Hansen ,Peter R Hobson ,Q Ingram,R Del Burgo,R Démina ,R Granier De Cassagnac,R I Rabadán-Trejo ,R López-Fernández ,R Taus,Raghav Kunnawalkam Elayavalli ,Ravindra Kumar Verma,Riccardo Andrea Manzoni ,S Abu Zeid,S Argirò ,S Czellár ,S Dubé ,S K Pflitsch,S Lacaprara,S Perriès ,S Slabospitskii,S Sánchez Cruz ,S Tkaczyk,S Çerçi ,S Đurić ,Sa Jain,Sandra S Padula,Sanjeev Kumar ,Seth Conrad Zenz ,Sh Jain,Shamik Ghosh ,Silvia Goy López ,Simranjit Singh Chhibra ,T Geralis,T Maënpaä ,T Tabarelli De Fatis,T Du Pree,T Šuša ,Tao Huang ,Thea Klaeboe Aarrestad ,Thomas Müller ,U K Yang,V Brigljević ,V Dūdėnas ,V Kutzner,V Lemaı̂tre ,V Monaco,V Myronenko,V Rodŕıguez Bouza ,V Veszprémi ,W Van Doninck,Wan Ahmad Tajuddin Wan Abdullah ,Wolfram Dietrich Zeuner ,Y Chào ,Y Güler ,Yang Yu ,Yu Andreev,Yu I Skovpen ,Yuan Li ,Z Shi ,Z Szillási ,Zainol Abidin Ibrahim ,Zhihao Xu ,A Abdulsalam,A Ackert,A Agapitos,A Ahmad,A Al-Bataineh,A Albert,A Apresyan,A Apyan,A Askew,A Attikis,A Babaev,A Baden,A Barker,A Baskakov,A Baty,A Bean,A Belloni,A Belyaev,A Benaglia,A Benecke,A Beretvas,A Bermúdez Martínez,A Beschi,A Bhardwaj,A Bocci,A Boletti,A Braghieri,A Brinkerhoff,A Buccilli,A Bundock,A Bylinkin,A Byszuk,A C Benvenuti,A C 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doi:10.1007/jhep08(2018)016

Abstract

A search is presented for long-lived charged particles that decay within the CMS detector and produce the signature of a disappearing track. A disappearing track is an isolated track with missing hits in the outer layers of the silicon tracker, little or no energy in associated calorimeter deposits, and no associated hits in the muon detectors. This search uses data collected with the CMS detector in 2015 and 2016 from proton-proton collisions at a center-of-mass energy of 13 TeV at the LHC, corresponding to an integrated luminosity of 38.4 fb−1. The results of the search are interpreted in the context of the anomaly-mediated supersymmetry breaking model. The data are consistent with the background-only hypothesis. Limits are set on the product of the cross section for direct production of charginos and their branching fraction to a neutralino and a pion, as a function of the chargino mass and lifetime. At 95% confidence level, charginos with masses below 715 (695) GeV are excluded for a lifetime of 3 (7) ns, as are charginos with lifetimes from 0.5 to 60 ns for a mass of 505 GeV. These are the most stringent limits using a disappearing track signature on this signal model for chargino lifetimes above ≈0.7 ns.

Highlights

Background estimation5.1 Charged leptonsThe dominant source of high-pT, isolated tracks from standard model (SM) processes arises from charged leptons from the decay of W or Z bosons or virtual photons
A search is presented for long-lived charged particles that decay within the CMS detector and produce the signature of a disappearing track
A disappearing track is an isolated track with missing hits in the outer layers of the silicon tracker, little or no energy in associated calorimeter deposits, and no associated hits in the muon detectors

Summary

The CMS detector

The central feature of the CMS apparatus is a superconducting solenoid of 6 m internal diameter. The silicon tracker measures charged particles within the pseudorapidity range |η| < 2.5 It consists of 1440 silicon pixel and 15 148 silicon strip detector modules and is located in the 3.8 T field of the solenoid. For particles that are not explicitly required to be isolated from other event activity, and that have transverse momentum 1 < pT < 10 GeV and |η| < 1.4, the track resolutions are typically 1.5% in pT and 25–90 (45–150) μm in the transverse (longitudinal) impact parameter. These particles represent the bulk of those produced in collisions. A more detailed description of the CMS detector, together with a definition of the coordinate system used and the relevant kinematic variables, can be found in ref. [19]

Data sets

Event reconstruction and selection

Charged leptons

Spurious tracks

Background estimates

Signal efficiencies

Results

Summary

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Journal: Journal of High Energy Physics	Publication Date: Aug 1, 2018
Citations: 48	License type: open-access

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Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at sqrt{s}=13 TeV

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Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at sqrt{s}=13 TeV

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