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Measurements of jet substructure describing the composition of quark- and gluon-initiated jets are presented. Proton-proton (pp) collision data at s = 13 TeV collected with the CMS detector are used, corresponding to an integrated luminosity of 35.9 fb−1. Generalized angularities are measured that characterize the jet substructure and distinguish quark- and gluon-initiated jets. These observables are sensitive to the distributions of transverse momenta and angular distances within a jet. The analysis is performed using a data sample of dijet events enriched in gluon-initiated jets, and, for the first time, a Z+jet event sample enriched in quark-initiated jets. The observables are measured in bins of jet transverse momentum, and as a function of the jet radius parameter. Each measurement is repeated applying a “soft drop” grooming procedure that removes soft and large angle radiation from the jet. Using these measurements, the ability of various models to describe jet substructure is assessed, showing a clear need for improvements in Monte Carlo generators.
Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Chatterjee, S., Dragicevic, M., et al. (2022). Study of quark and gluon jet substructure in Z+jet and dijet events from pp collisions. JOURNAL OF HIGH ENERGY PHYSICS, 2022(1) [10.1007/jhep01(2022)188].
Study of quark and gluon jet substructure in Z+jet and dijet events from pp collisions
A. Tumasyan;W. Adam;J. W. Andrejkovic;T. Bergauer;S. Chatterjee;M. Dragicevic;A. Escalante Del Valle;R. Fr??hwirth;M. Jeitler;N. Krammer;L. Lechner;D. Liko;I. Mikulec;P. Paulitsch;F. M. Pitters;J. Schieck;R. Sch??fbeck;M. Spanring;S. Templ;W. Waltenberger;C. -E. Wulz;V. Chekhovsky;A. Litomin;V. Makarenko;M. R. Darwish;E. A. De Wolf;T. Janssen;T. Kello;A. Lelek;H. Rejeb Sfar;P. Van Mechelen;S. Van Putte;N. Van Remortel;F. Blekman;E. S. Bols;J. D???Hondt;M. Delcourt;H. El Faham;S. Lowette;S. Moortgat;A. Morton;D. M??ller;A. R. Sahasransu;S. Tavernier;W. Van Doninck;P. Van Mulders;D. Beghin;B. Bilin;B. Clerbaux;G. De Lentdecker;L. Favart;A. Grebenyuk;A. K. Kalsi;K. Lee;M. Mahdavikhorrami;I. Makarenko;L. Moureaux;L. P??tr??;A. Popov;N. Postiau;E. Starling;L. Thomas;M. Vanden Bemden;C. Vander Velde;P. Vanlaer;D. Vannerom;L. Wezenbeek;T. Cornelis;D. Dobur;J. Knolle;L. Lambrecht;G. Mestdach;M. Niedziela;C. Roskas;A. Samalan;K. Skovpen;M. Tytgat;W. Verbeke;B. Vermassen;M. Vit;A. Bethani;G. 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Chapon;G. M. Chen;H. S. Chen;M. Chen;F. Iemmi;A. Kapoor;D. Leggat;H. Liao;Z. -A. LIU;V. Milosevic;F. Monti;R. Sharma;J. Tao;J. Thomas-wilsker;J. Wang;H. Zhang;S. Zhang;J. Zhao;A. Agapitos;Y. An;Y. Ban;C. Chen;A. Levin;Q. Li;X. Lyu;Y. Mao;S. J. Qian;D. Wang;Q. Wang;J. Xiao;M. Lu;Z. You;X. Gao;H. Okawa;Z. Lin;M. Xiao;C. Avila;A. Cabrera;C. Florez;J. Fraga;J. Mejia Guisao;F. Ramirez;J. D. Ruiz Alvarez;C. A. Salazar Gonz??lez;D. Giljanovic;N. Godinovic;D. Lelas;I. Puljak;Z. Antunovic;M. Kovac;T. Sculac;V. Brigljevic;D. Ferencek;D. Majumder;M. Roguljic;A. Starodumov;T. Susa;A. Attikis;K. Christoforou;E. Erodotou;A. Ioannou;G. Kole;M. Kolosova;S. Konstantinou;J. Mousa;C. Nicolaou;F. Ptochos;P. A. Razis;H. Rykaczewski;H. Saka;M. Finger;M. Finger;A. Kveton;E. Ayala;E. Carrera Jarrin;H. Abdalla;S. Abu Zeid;M. A. Mahmoud;Y. Mohammed;S. Bhowmik;R. K. Dewanjee;K. Ehataht;M. Kadastik;S. Nandan;C. Nielsen;J. Pata;M. Raidal;L. Tani;C. Veelken;P. Eerola;L. Forthomme;H. Kirschenmann;K. Osterberg;M. 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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;F. Meng;K. Mohrman;Y. Musienko;R. Ruchti;P. Siddireddy;A. Townsend;M. Wayne;A. Wightman;M. Wolf;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;M. T. Lucchini;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;M. Liu;G. Negro;N. Neumeister;G. Paspalaki;C. C. Peng;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;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
Measurements of jet substructure describing the composition of quark- and gluon-initiated jets are presented. Proton-proton (pp) collision data at s = 13 TeV collected with the CMS detector are used, corresponding to an integrated luminosity of 35.9 fb−1. Generalized angularities are measured that characterize the jet substructure and distinguish quark- and gluon-initiated jets. These observables are sensitive to the distributions of transverse momenta and angular distances within a jet. The analysis is performed using a data sample of dijet events enriched in gluon-initiated jets, and, for the first time, a Z+jet event sample enriched in quark-initiated jets. The observables are measured in bins of jet transverse momentum, and as a function of the jet radius parameter. Each measurement is repeated applying a “soft drop” grooming procedure that removes soft and large angle radiation from the jet. Using these measurements, the ability of various models to describe jet substructure is assessed, showing a clear need for improvements in Monte Carlo generators.
Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Chatterjee, S., Dragicevic, M., et al. (2022). Study of quark and gluon jet substructure in Z+jet and dijet events from pp collisions. JOURNAL OF HIGH ENERGY PHYSICS, 2022(1) [10.1007/jhep01(2022)188].
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/10281/415016
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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 598/2018 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.