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Search for a third-generation leptoquark coupled to a τ lepton and a b quark through single, pair, and nonresonant production in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV

A. HayrapetyanInstitut f ür Hochenergiephysik, Vienna, AustriaA. TumasyanYerevan Physics Institute, Yerevan, ArmeniaW. AdamUniversiteit Antwerpen, Antwerpen, BelgiumJanik Walter AndrejkovicInstitut für HochenergiephysikT. BergauerYerevan Physics Institute, Yerevan, ArmeniaS. ChatterjeeInstitut f ür Hochenergiephysik, Vienna, AustriaK. DamanakisInstitut f ür Hochenergiephysik, Vienna, AustriaM. DragicevicInstitut für HochenergiephysikA. Escalante Del ValleInstitut für HochenergiephysikPriya Sajid HussainYerevan Physics Institute, Yerevan, ArmeniaM. JeitlerTU WienNatascha KrammerInstitut für HochenergiephysikD. LikoInstitut für HochenergiephysikI. MikulecInstitut für HochenergiephysikJ. SchieckTU WienR. SchöfbeckInstitut f ür Hochenergiephysik, Vienna, AustriaD. SchwarzUniversiteit Antwerpen, Antwerpen, BelgiumM. SonawaneInstitut für HochenergiephysikS. TemplInstitut f ür Hochenergiephysik, Vienna, AustriaW. WaltenbergerYerevan Physics Institute, Yerevan, ArmeniaC.-E. WulzTU WienM. R. DarwishArab Academy for Science, Technology and Maritime TransportX. JanssenUniversiteit Antwerpen, Antwerpen, BelgiumP. Van MechelenYerevan Physics Institute, Yerevan, ArmeniaE. S. BolsVrije Universiteit BrusselJ. D’HondtUniversiteit Antwerpen, Antwerpen, BelgiumSoumya DansanaVrije Universiteit BrusselA. De MoorVrije Universiteit BrusselM. DelcourtYerevan Physics Institute, Yerevan, ArmeniaH. El FahamVrije Universiteit BrusselS. LowetteYerevan Physics Institute, Yerevan, ArmeniaI. MakarenkoVrije Universiteit BrusselD. MüllerInstitut f ür Hochenergiephysik, Vienna, AustriaA. R. SahasransuInstitut f ür Hochenergiephysik, Vienna, AustriaS. TavernierInstitut f ür Hochenergiephysik, Vienna, AustriaM. TytgatGhent UniversityS. Van PutteInstitut f ür Hochenergiephysik, Vienna, AustriaD. VanneromYerevan Physics Institute, Yerevan, ArmeniaB. ClerbauxUniversité Libre de BruxellesG. De LentdeckerYerevan Physics Institute, Yerevan, ArmeniaL. FavartInstitut f ür Hochenergiephysik, Vienna, AustriaD. HohovUniversiteit Antwerpen, Antwerpen, BelgiumJ. JaramilloUniversiteit Antwerpen, Antwerpen, BelgiumA. KhalilzadehYerevan Physics Institute, Yerevan, ArmeniaK. LeeKorea UniversityM. MahdavikhorramiUniversité Libre de BruxellesA. MalaraInstitut f ür Hochenergiephysik, Vienna, AustriaS. ParedesUniversité Libre de BruxellesL. PétréUniversité Libre de BruxellesN. PostiauUniversiteit Antwerpen, Antwerpen, BelgiumLaurent ThomasUniversiteit Antwerpen, Antwerpen, BelgiumM. Vanden BemdenUniversité Libre de BruxellesC. Vander VeldeInstitut f ür Hochenergiephysik, Vienna, AustriaP. VanlaerUniversiteit Antwerpen, Antwerpen, BelgiumM. De CoenUniversiteit Antwerpen, Antwerpen, BelgiumD. DoburGhent UniversityY. HongInstitut f ür Hochenergiephysik, Vienna, AustriaJ. KnolleGhent UniversityLuka LambrechtInstitut f ür Hochenergiephysik, Vienna, AustriaG. MestdachGhent UniversityCésar RendónInstitut f ür Hochenergiephysik, Vienna, AustriaA. SamalanYerevan Physics Institute, Yerevan, ArmeniaK. SkovpenGhent UniversityN. Van Den BosscheGhent UniversityLiam WezenbeekYerevan Physics Institute, Yerevan, ArmeniaA. BeneckeUniversité Catholique de LouvainG. BrunoUniversiteit Antwerpen, Antwerpen, BelgiumC. CaputoUniversité Catholique de LouvainC. DelaereUniversiteit Antwerpen, Antwerpen, BelgiumI. S. DonertasUniversité Catholique de LouvainA. GiammancoUniversité Catholique de LouvainK. JaffelYerevan Physics Institute, Yerevan, ArmeniaSa. JainUniversiteit Antwerpen, Antwerpen, BelgiumV. LemaitreInstitut f ür Hochenergiephysik, Vienna, AustriaPaola MastrapasquaInstitut f ür Hochenergiephysik, Vienna, AustriaK. MondalUniversité Catholique de LouvainT. T. TranInstitut f ür Hochenergiephysik, Vienna, AustriaS. WertzUniversité Catholique de LouvainG. A. AlvesCentro Brasileiro de Pesquisas FisicasE. CoelhoCentro Brasileiro de Pesquisas FisicasC. HenselYerevan Physics Institute, Yerevan, ArmeniaT. Menezes De OliveiraYerevan Physics Institute, Yerevan, ArmeniaA. MoraesInstitut f ür Hochenergiephysik, Vienna, AustriaP. Rebello TelesUniversiteit Antwerpen, Antwerpen, BelgiumM. SoeiroCentro Brasileiro de Pesquisas FisicasW. L. Aldá JúniorUniversidade do Estado do Rio de JaneiroM. Alves Gallo PereiraUniversidade do Estado do Rio de JaneiroM. Barroso Ferreira FilhoUniversiteit Antwerpen, Antwerpen, BelgiumH. Brandao MalbouissonYerevan Physics Institute, Yerevan, ArmeniaW. CarvalhoUniversiteit Antwerpen, Antwerpen, BelgiumJ. ChinellatoYerevan Physics Institute, Yerevan, ArmeniaE. M. Da CostaYerevan Physics Institute, Yerevan, ArmeniaG. G. Da SilveiraUniversidade do Estado do Rio de JaneiroD. De Jesus DamiãoYerevan Physics Institute, Yerevan, ArmeniaS. Fonseca De SouzaUniversiteit Antwerpen, Antwerpen, BelgiumJ. MartinsUFMSC. Mora HerreraCentro de Investigacion y de Estudios Avanzados del IPNK. Mota AmariloUniversidade do Estado do Rio de JaneiroL. MundimInstitut f ür Hochenergiephysik, Vienna, Austria
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A bstract A search is presented for a third-generation leptoquark (LQ) coupled exclusively to a τ lepton and a b quark. The search is based on proton-proton collision data at a center-of-mass energy of 13 TeV recorded with the CMS detector, corresponding to an integrated luminosity of 138 fb − 1 . Events with τ leptons and a varying number of jets originating from b quarks are considered, targeting the single and pair production of LQs, as well as nonresonant t -channel LQ exchange. An excess is observed in the data with respect to the background expectation in the combined analysis of all search regions. For a benchmark LQ mass of 2 TeV and an LQ-b-τ coupling strength of 2.5, the excess reaches a local significance of up to 2.8 standard deviations. Upper limits at the 95% confidence level are placed on the LQ production cross section in the LQ mass range 0.5–2.3 TeV, and up to 3 TeV for t -channel LQ exchange. Leptoquarks are excluded below masses of 1.22–1.88 TeV for different LQ models and varying coupling strengths up to 2.5. The study of nonresonant ττ production through t -channel LQ exchange allows lower limits on the LQ mass of up to 2.3 TeV to be obtained.

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