Search for excited tau leptons in the ττγ final state in proton-proton collisions at = 13 TeV
Özet
Results are presented for a test of the compositeness of the heaviest charged lepton, τ, using data collected by the CMS experiment in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC. The data were collected in 2016–2018 and correspond to an integrated luminosity of 138 fb−1. This analysis searches for tau lepton pair production in which one of the tau leptons is produced in an excited state and decays to a ground state tau lepton and a photon. The event selection consists of two isolated tau lepton decay candidates and a high-energy photon. The mass of the excited tau lepton is reconstructed using the missing transverse momentum in the event, assuming the momentum of the neutrinos from each tau lepton decay are aligned with the visible decay products. No excess of events above the standard model background prediction is observed. This null result is used to set lower bounds on the excited tau lepton mass. For a compositeness scale Λ equal to the excited tau lepton mass, excited tau leptons with masses below 4700 GeV are excluded at 95% confidence level; for Λ = 10 TeV this exclusion is set at 2800 GeV. This is the first experimental result covering this production and decay process in the excited tau mass range above 175 GeV. © The Author(s) 2025.
Anahtar Kelimeler
Tam Kayıt
| Alan | Değer | Dil |
|---|---|---|
| dc.contributor.author | Hayrapetyan, A. | |
| dc.contributor.author | Tumasyan, A. | |
| dc.contributor.author | Adam, W. | |
| dc.contributor.author | Andrejkovic, J.W. | |
| dc.contributor.author | Benato, L. | |
| dc.contributor.author | Bergauer, T. | |
| dc.contributor.author | Chatterjee, S. | |
| dc.contributor.author | Damanakis, K. | |
| dc.contributor.author | Dragicevic, M. | |
| dc.contributor.author | Hussain, P.S. | |
| dc.contributor.author | Jeitler, M. | |
| dc.contributor.author | Krammer, N. | |
| dc.contributor.author | Li, A. | |
| dc.contributor.author | Liko, D. | |
| dc.contributor.author | Mikulec, I. | |
| dc.contributor.author | Schieck, J. | |
| dc.contributor.author | Schöfbeck, R. | |
| dc.contributor.author | Schwarz, D. | |
| dc.contributor.author | Sonawane, M. | |
| dc.contributor.author | Waltenberger, W. | |
| dc.contributor.author | Wulz, C.-E. | |
| dc.contributor.author | Janssen, T. | |
| dc.contributor.author | Van Laer, T. | |
| dc.contributor.author | Van Mechelen, P. | |
| dc.contributor.author | Breugelmans, N. | |
| dc.contributor.author | D’Hondt, J. | |
| dc.contributor.author | Dansana, S. | |
| dc.contributor.author | De Moor, A. | |
| dc.contributor.author | Delcourt, M. | |
| dc.contributor.author | Heyen, F. | |
| dc.contributor.author | Lowette, S. | |
| dc.contributor.author | Makarenko, I. | |
| dc.contributor.author | Müller, D. | |
| dc.contributor.author | Tavernier, S. | |
| dc.contributor.author | Tytgat, M. | |
| dc.contributor.author | Van Onsem, G.P. | |
| dc.contributor.author | Van Putte, S. | |
| dc.contributor.author | Vannerom, D. | |
| dc.contributor.author | Bilin, B. | |
| dc.contributor.author | Clerbaux, B. | |
| dc.contributor.author | Das, A.K. | |
| dc.contributor.author | De Bruyn, I. | |
| dc.contributor.author | De Lentdecker, G. | |
| dc.contributor.author | Evard, H. | |
| dc.contributor.author | Favart, L. | |
| dc.contributor.author | Gianneios, P. | |
| dc.contributor.author | Jaramillo, J. | |
| dc.contributor.author | Khalilzadeh, A. | |
| dc.contributor.author | Khan, F.A. | |
| dc.contributor.author | Lee, K. | |
| dc.date.accessioned | 2026-10-18T20:26:01.574234621Z | |
| dc.date.available | 2026-10-18T20:26:01.574234621Z | |
| dc.date.issued | 2025 | |
| dc.description.abstract | Results are presented for a test of the compositeness of the heaviest charged lepton, τ, using data collected by the CMS experiment in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC. The data were collected in 2016–2018 and correspond to an integrated luminosity of 138 fb−1. This analysis searches for tau lepton pair production in which one of the tau leptons is produced in an excited state and decays to a ground state tau lepton and a photon. The event selection consists of two isolated tau lepton decay candidates and a high-energy photon. The mass of the excited tau lepton is reconstructed using the missing transverse momentum in the event, assuming the momentum of the neutrinos from each tau lepton decay are aligned with the visible decay products. No excess of events above the standard model background prediction is observed. This null result is used to set lower bounds on the excited tau lepton mass. For a compositeness scale Λ equal to the excited tau lepton mass, excited tau leptons with masses below 4700 GeV are excluded at 95% confidence level; for Λ = 10 TeV this exclusion is set at 2800 GeV. This is the first experimental result covering this production and decay process in the excited tau mass range above 175 GeV. © The Author(s) 2025. | |
| dc.description.sponsorship | We congratulate our colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS effort. In addition, we gratefully acknowledge the computing centers and personnel of the Worldwide LHC Computing Grid and other centers for delivering so effectively the computing infrastructure essential to our analyses. Finally, we acknowledge the enduring support for the construction and operation of the LHC, the CMS detector, and the supporting computing infrastructure provided by the following funding agencies: SC (Armenia), BMBWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, FAPERGS, and FAPESP (Brazil); MES and BNSF (Bulgaria); CERN; CAS, MoST, and NSFC (China); MINCIENCIAS (Colombia); MSES and CSF (Croatia); RIF (Cyprus); SENESCYT (Ecuador); ERC PRG, RVTT3 and MoER TK202 (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); SRNSF (Georgia); BMBF, DFG, and HGF (Germany); GSRI (Greece); NKFIH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); MSIP and NRF (Republic of Korea); MES (Latvia); LMTLT (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MOS (Montenegro); MBIE (New Zealand); PAEC (Pakistan); MES and NSC (Poland); FCT (Portugal); MESTD (Serbia); MCIN/AEI and PCTI (Spain); MOSTR (Sri Lanka); Swiss Funding Agencies (Switzerland); MST (Taipei); MHESI and NSTDA (Thailand); TUBITAK and TENMAK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (U.S.A.). | |
| dc.identifier.doi | 10.1007/jhep06(2025)006 | |
| dc.identifier.issn | 1029-8479 | |
| dc.identifier.issue | 6 | |
| dc.identifier.scopus | 2-s2.0-105012496802 | |
| dc.identifier.startpage | 6 | |
| dc.identifier.uri | https://rdlopen.rawdatalibrary.net/r/ebyu/10916 | |
| dc.identifier.volume | 2025 | |
| dc.language.iso | en | |
| dc.publisher | Springer Science and Business Media Deutschland GmbH | |
| dc.relation.ispartof | Journal of High Energy Physics | |
| dc.rights | info:eu-repo/semantics/openAccess | |
| dc.subject | Beyond Standard Model | |
| dc.subject | Hadron-Hadron Scattering | |
| dc.subject | Tau Physics | |
| dc.title | Search for excited tau leptons in the ττγ final state in proton-proton collisions at = 13 TeV | |
| dc.type | Article | |
| dspace.entity.type | Publication | |
| rdl.citation.scopus | 5 | |
| rdl.oa.status | gold | |
| rdl.source.index | SCOPUS |
