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Results are presented from a search for charged-lepton flavor violating (CLFV) interactions in top quark production and decay in pp collisions at a center-of-mass energy of 13 TeV. The events are required to contain one oppositely charged electron-muon pair in the final state, along with at least one jet identified as originating from a bottom quark. The data correspond to an integrated luminosity of 138 fb(-1), collected by the CMS experiment at the LHC. This analysis includes both the production (q -> e mu t) and decay (t -> e mu q) modes of the top quark through CLFV interactions, with q referring to a u or c quark. These interactions are parametrized using an effective field theory approach. With no significant excess over the standard model expectation, the results are interpreted in terms of vector-, scalar-, and tensor-like CLFV four-fermion effective interactions. Finally, observed exclusion limits are set at 95% confidence levels on the respective branching fractions of a top quark to an e mu pair and an up (charm) quark of 0.13 x 10(-6) (1.31 x 10(-6)), 0.07 x 10(-6) (0.89 x 10(-6)), and 0.25 x 10(-6) (2.59 x 10(-6)) for vector, scalar, and tensor CLFV interactions, respectively.
Search for charged-lepton flavor violation in top quark production and decay in pp collisions at $$ \sqrt{s} $$ = 13 TeV
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Cheung;F. Chlebana;M. Cremonesi;K. F. Di Petrillo;V. D. Elvira;Y. Feng;J. Freeman;Z. Gecse;L. Gray;D. Green;S. Gr??nendahl;O. Gutsche;R. M. Harris;R. Heller;T. C. Herwig;J. Hirschauer;B. Jayatilaka;S. Jindariani;M. Johnson;U. Joshi;T. Klijnsma;B. Klima;K. H. M. Kwok;S. Lammel;D. Lincoln;R. Lipton;T. Liu;C. Madrid;K. Maeshima;C. Mantilla;D. Mason;P. McBride;P. Merkel;S. Mrenna;S. Nahn;J. Ngadiuba;V. O???Dell;V. Papadimitriou;K. Pedro;C. Pena;O. Prokofyev;F. Ravera;A. Reinsvold Hall;L. Ristori;E. Sexton-Kennedy;N. Smith;A. Soha;W. J. Spalding;L. Spiegel;S. Stoynev;J. Strait;L. Taylor;S. Tkaczyk;N. V. Tran;L. Uplegger;E. W. Vaandering;H. A. Weber;D. Acosta;P. Avery;D. Bourilkov;L. Cadamuro;V. Cherepanov;F. Errico;R. D. Field;D. Guerrero;B. M. Joshi;M. Kim;E. Koenig;J. Konigsberg;A. Korytov;K. H. Lo;K. Matchev;N. Menendez;G. Mitselmakher;A. Muthirakalayil Madhu;N. Rawal;D. Rosenzweig;S. Rosenzweig;J. Rotter;K. Shi;J. Sturdy;J. Wang;E. Yigitbasi;X. Zuo;T. Adams;A. Askew;R. Habibullah;V. 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Tapia Takaki;Q. Wang;Z. Warner;J. Williams;G. Wilson;S. Duric;A. Ivanov;K. Kaadze;D. Kim;Y. Maravin;T. Mitchell;A. Modak;K. Nam;F. Rebassoo;D. Wright;E. Adams;A. Baden;O. Baron;A. Belloni;S. C. Eno;N. J. Hadley;S. Jabeen;R. G. Kellogg;T. Koeth;A. C. Mignerey;S. Nabili;C. Palmer;M. Seidel;A. Skuja;L. Wang;K. Wong;D. Abercrombie;G. Andreassi;R. Bi;S. Brandt;W. Busza;I. A. Cali;Y. Chen;M. D???Alfonso;J. Eysermans;C. Freer;G. Gomez Ceballos;M. Goncharov;P. Harris;M. Hu;M. Klute;D. Kovalskyi;J. Krupa;Y. -J. Lee;C. Mironov;C. Paus;D. Rankin;C. Roland;G. Roland;Z. Shi;G. S. F. Stephans;J. Wang;Z. Wang;B. Wyslouch;R. M. Chatterjee;A. Evans;P. Hansen;J. Hiltbrand;Sh. Jain;M. Krohn;Y. Kubota;J. Mans;M. Revering;R. Rusack;R. Saradhy;N. Schroeder;N. Strobbe;M. A. Wadud;K. Bloom;M. Bryson;S. Chauhan;D. R. Claes;C. Fangmeier;L. Finco;F. Golf;C. Joo;I. Kravchenko;M. Musich;I. Reed;J. E. Siado;G. R. Snow;W. Tabb;F. Yan;A. G. Zecchinelli;G. Agarwal;H. Bandyopadhyay;L. Hay;I. Iashvili;A. Kharchilava;C. McLean;D. Nguyen;J. Pekkanen;S. Rappoccio;A. Williams;G. Alverson;E. Barberis;Y. Haddad;A. Hortiangtham;J. Li;G. Madigan;B. Marzocchi;D. M. Morse;V. Nguyen;T. Orimoto;A. Parker;L. Skinnari;A. Tishelman-Charny;T. Wamorkar;B. Wang;A. Wisecarver;D. Wood;S. Bhattacharya;J. Bueghly;Z. Chen;A. Gilbert;T. Gunter;K. A. Hahn;Y. Liu;N. Odell;M. H. Schmitt;M. Velasco;R. Band;R. Bucci;A. Das;N. Dev;R. Goldouzian;M. Hildreth;K. Hurtado Anampa;C. Jessop;K. Lannon;J. Lawrence;N. Loukas;D. Lutton;N. Marinelli;I. Mcalister;T. McCauley;C. Mcgrady;K. Mohrman;Y. Musienko;R. Ruchti;P. Siddireddy;A. Townsend;M. Wayne;A. Wightman;M. Zarucki;L. Zygala;B. Bylsma;B. Cardwell;L. S. Durkin;B. Francis;C. Hill;M. Nunez Ornelas;K. Wei;B. L. Winer;B. R. Yates;F. M. Addesa;B. Bonham;P. Das;G. Dezoort;P. Elmer;A. Frankenthal;B. Greenberg;N. Haubrich;S. Higginbotham;A. Kalogeropoulos;G. Kopp;S. Kwan;D. Lange;D. Marlow;K. Mei;I. Ojalvo;J. Olsen;D. Stickland;C. Tully;S. Malik;S. Norberg;A. S. Bakshi;V. E. Barnes;R. Chawla;S. Das;L. Gutay;M. Jones;A. W. Jung;S. Karmarkar;D. Kondratyev;M. Liu;G. Negro;N. Neumeister;G. Paspalaki;S. Piperov;A. Purohit;J. F. Schulte;M. Stojanovic;J. Thieman;F. Wang;R. Xiao;W. Xie;J. Dolen;N. Parashar;A. Baty;M. Decaro;S. Dildick;K. M. Ecklund;S. Freed;P. Gardner;F. J. M. Geurts;A. Kumar;W. Li;B. P. Padley;R. Redjimi;W. Shi;A. G. Stahl Leiton;S. Yang;L. Zhang;Y. Zhang;A. Bodek;P. de Barbaro;R. Demina;J. L. Dulemba;C. Fallon;T. Ferbel;M. Galanti;A. Garcia-Bellido;O. Hindrichs;A. Khukhunaishvili;E. Ranken;R. Taus;B. Chiarito;J. P. Chou;A. Gandrakota;Y. Gershtein;E. Halkiadakis;A. Hart;M. Heindl;O. Karacheban;I. Laflotte;A. Lath;R. Montalvo;K. Nash;M. Osherson;S. Salur;S. Schnetzer;S. Somalwar;R. Stone;S. A. Thayil;S. Thomas;H. Wang;H. Acharya;A. G. Delannoy;S. Fiorendi;S. Spanier;O. Bouhali;M. Dalchenko;A. Delgado;R. Eusebi;J. Gilmore;T. Huang;T. Kamon;H. Kim;S. Luo;S. Malhotra;R. Mueller;D. Overton;D. Rathjens;A. Safonov;N. Akchurin;J. Damgov;V. Hegde;S. Kunori;K. Lamichhane;S. W. Lee;T. Mengke;S. Muthumuni;T. Peltola;I. Volobouev;Z. Wang;A. Whitbeck;E. Appelt;S. Greene;A. Gurrola;W. Johns;A. Melo;H. Ni;K. Padeken;F. Romeo;P. Sheldon;S. Tuo;J. Velkovska;M. W. Arenton;B. Cox;G. Cummings;J. Hakala;R. Hirosky;M. Joyce;A. Ledovskoy;A. Li;C. Neu;C. E. Perez Lara;B. Tannenwald;S. White;E. Wolfe;N. Poudyal;K. Black;T. Bose;C. Caillol;S. Dasu;I. De Bruyn;P. Everaerts;F. Fienga;C. Galloni;H. He;M. Herndon;A. Herv??;U. Hussain;A. Lanaro;A. Loeliger;R. Loveless;J. Madhusudanan Sreekala;A. Mallampalli;A. Mohammadi;D. Pinna;A. Savin;V. Shang;V. Sharma;W. H. Smith;D. Teague;S. Trembath-Reichert;W. Vetens
2022
Abstract
Results are presented from a search for charged-lepton flavor violating (CLFV) interactions in top quark production and decay in pp collisions at a center-of-mass energy of 13 TeV. The events are required to contain one oppositely charged electron-muon pair in the final state, along with at least one jet identified as originating from a bottom quark. The data correspond to an integrated luminosity of 138 fb(-1), collected by the CMS experiment at the LHC. This analysis includes both the production (q -> e mu t) and decay (t -> e mu q) modes of the top quark through CLFV interactions, with q referring to a u or c quark. These interactions are parametrized using an effective field theory approach. With no significant excess over the standard model expectation, the results are interpreted in terms of vector-, scalar-, and tensor-like CLFV four-fermion effective interactions. Finally, observed exclusion limits are set at 95% confidence levels on the respective branching fractions of a top quark to an e mu pair and an up (charm) quark of 0.13 x 10(-6) (1.31 x 10(-6)), 0.07 x 10(-6) (0.89 x 10(-6)), and 0.25 x 10(-6) (2.59 x 10(-6)) for vector, scalar, and tensor CLFV interactions, respectively.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11391/1547736
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simulazione ASN
Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande.
La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.