Measurement of the top quark mass using a profile likelihood approach with the lepton + jets final states in proton–proton collisions at √s=13TeV
ArticleAçık Erişim
Özet
The mass of the top quark is measured in 36.3 fb-1 of LHC proton–proton collision data collected with the CMS detector at s=13TeV . The measurement uses a sample of top quark pair candidate events containing one isolated electron or muon and at least four jets in the final state. For each event, the mass is reconstructed from a kinematic fit of the decay products to a top quark pair hypothesis. A profile likelihood method is applied using up to four observables per event to extract the top quark mass. The top quark mass is measured to be 171.77±0.37GeV . This approach significantly improves the precision over previous measurements. © 2023, The Author(s).
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RDL Kalıcı Bağlantı (PID)
https://rdlopen.rawdatalibrary.net/r/ebyu/11658Resmi atıflarda kullanılan kalıcı adresTam Kayıt
| Alan | Değer | Dil |
|---|---|---|
| dc.contributor.author | Tumasyan, A. | |
| dc.contributor.author | Adam, W. | |
| dc.contributor.author | Andrejkovic, J.W. | |
| dc.contributor.author | Bergauer, T. | |
| dc.contributor.author | Chatterjee, S. | |
| dc.contributor.author | Damanakis, K. | |
| dc.contributor.author | Dragicevic, M. | |
| dc.contributor.author | Del Valle, A. Escalante | |
| dc.contributor.author | Hussain, P.S. | |
| dc.contributor.author | Jeitler, M. | |
| dc.contributor.author | Krammer, N. | |
| dc.contributor.author | Lechner, L. | |
| dc.contributor.author | Liko, D. | |
| dc.contributor.author | Mikulec, I. | |
| dc.contributor.author | Paulitsch, P. | |
| dc.contributor.author | Pitters, F.M. | |
| dc.contributor.author | Schieck, J. | |
| dc.contributor.author | Schöfbeck, R. | |
| dc.contributor.author | Schwarz, D. | |
| dc.contributor.author | Sonawane, M. | |
| dc.contributor.author | Templ, S. | |
| dc.contributor.author | Waltenberger, W. | |
| dc.contributor.author | Wulz, C.-E. | |
| dc.contributor.author | Darwish, M.R. | |
| dc.contributor.author | Janssen, T. | |
| dc.contributor.author | Kello, T. | |
| dc.contributor.author | Sfar, H. Rejeb | |
| dc.contributor.author | Van Mechelen, P. | |
| dc.contributor.author | Bols, E.S. | |
| dc.contributor.author | D’Hondt, J. | |
| dc.contributor.author | De Moor, A. | |
| dc.contributor.author | Delcourt, M. | |
| dc.contributor.author | El Faham, H. | |
| dc.contributor.author | Lowette, S. | |
| dc.contributor.author | Moortgat, S. | |
| dc.contributor.author | Morton, A. | |
| dc.contributor.author | Müller, D. | |
| dc.contributor.author | Sahasransu, A.R. | |
| dc.contributor.author | Tavernier, S. | |
| dc.contributor.author | Van Doninck, W. | |
| dc.contributor.author | Vannerom, D. | |
| dc.contributor.author | Clerbaux, B. | |
| dc.contributor.author | De Lentdecker, G. | |
| dc.contributor.author | Favart, L. | |
| dc.contributor.author | Hohov, D. | |
| dc.contributor.author | Jaramillo, J. | |
| dc.contributor.author | Lee, K. | |
| dc.contributor.author | Mahdavikhorrami, M. | |
| dc.contributor.author | Makarenko, I. | |
| dc.contributor.author | Malara, A. | |
| dc.date.accessioned | 2026-10-18T20:26:40.646328513Z | |
| dc.date.available | 2026-10-18T20:26:40.646328513Z | |
| dc.date.issued | 2023 | |
| dc.description.abstract | The mass of the top quark is measured in 36.3 fb-1 of LHC proton–proton collision data collected with the CMS detector at s=13TeV . The measurement uses a sample of top quark pair candidate events containing one isolated electron or muon and at least four jets in the final state. For each event, the mass is reconstructed from a kinematic fit of the decay products to a top quark pair hypothesis. A profile likelihood method is applied using up to four observables per event to extract the top quark mass. The top quark mass is measured to be 171.77±0.37GeV . This approach significantly improves the precision over previous measurements. © 2023, The Author(s). | |
| dc.description.sponsorship | Science and Technology Facilities Council, STFC, (ST/X000583/1); Science and Technology Facilities Council, STFC; Horizon 2020 Framework Programme, H2020, (884104); Horizon 2020 Framework Programme, H2020 | |
| dc.identifier.doi | 10.1140/epjc/s10052-023-12050-4 | |
| dc.identifier.issn | 1434-6044 | |
| dc.identifier.issue | 10 | |
| dc.identifier.pmcid | PMC10600315 | |
| dc.identifier.pmid | 37906635 | |
| dc.identifier.scopus | 2-s2.0-85174914881 | |
| dc.identifier.startpage | 963 | |
| dc.identifier.uri | https://rdlopen.rawdatalibrary.net/r/ebyu/11658 | |
| dc.identifier.volume | 83 | |
| dc.language.iso | en | |
| dc.publisher | Institute for Ionics | |
| dc.relation.ispartof | European Physical Journal C | |
| dc.rights | info:eu-repo/semantics/openAccess | |
| dc.subject | CMS detectors | |
| dc.subject | Decay products | |
| dc.subject | Final state | |
| dc.subject | Likelihood methods | |
| dc.subject | Measurements of | |
| dc.subject | Profile likelihood | |
| dc.subject | Proton proton collisions | |
| dc.subject | Quark mass | |
| dc.subject | Top quarks | |
| dc.subject | Elementary particles | |
| dc.title | Measurement of the top quark mass using a profile likelihood approach with the lepton + jets final states in proton–proton collisions at √s=13TeV | |
| dc.type | Article | |
| dspace.entity.type | Publication | |
| rdl.citation.scopus | 27 | |
| rdl.department | Erzincan Binali Yildirim University, Erzincan, Turkey. | |
| rdl.oa.status | gold | |
| rdl.source.index | SCOPUS | |
| rdl.source.index | PUBMED |
