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The cross section for tt¯ production in the all-jets final state is measured in pp collisions at a centre-of-mass energy of 8 TeV at the LHC with the CMS detector, in data corresponding to an integrated luminosity of 18.4 fb−1. The inclusive cross section is found to be 275.6±6.1(stat)±37.8(syst)±7.2(lumi) ,pb. The normalized differential cross sections are measured as a function of the top quark transverse momenta, pT, and compared to predictions from quantum chromodynamics. The results are reported at detector, parton, and particle levels. In all cases, the measured top quark pT spectra are significantly softer than theoretical predictions.
(2016). Measurement of the tt¯ production cross section in the all-jets final state in pp collisions at √s = 8 TeV [journal article - articolo]. In THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS. Retrieved from http://hdl.handle.net/10446/140522
Measurement of the tt¯ production cross section in the all-jets final state in pp collisions at √s = 8 TeV
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D’Alfonso;D. d’Enterria;A. Dabrowski;V. Daponte;A. David;M. De Gruttola;F. De Guio;A. De Roeck;S. De Visscher;E. Di Marco;M. Dobson;M. Dordevic;B. Dorney;T. du Pree;M. Dünser;N. Dupont;A. Elliott-Peisert;G. Franzoni;W. Funk;D. Gigi;K. Gill;D. Giordano;M. Girone;F. Glege;R. Guida;S. Gundacker;M. Guthoff;J. Hammer;P. Harris;J. Hegeman;V. Innocente;P. Janot;H. Kirschenmann;M. J. Kortelainen;K. Kousouris;K. Krajczar;P. Lecoq;C. Lourenço;M. T. Lucchini;N. Magini;L. Malgeri;M. Mannelli;A. Martelli;L. Masetti;F. Meijers;S. Mersi;E. Meschi;F. Moortgat;S. Morovic;M. Mulders;M. V. Nemallapudi;H. Neugebauer;S. Orfanelli;L. Orsini;L. Pape;E. Perez;M. Peruzzi;A. Petrilli;G. Petrucciani;A. Pfeiffer;D. Piparo;A. Racz;G. Rolandi;M. Rovere;M. Ruan;H. Sakulin;C. Schäfer;C. Schwick;A. Sharma;P. Silva;M. Simon;P. Sphicas;J. Steggemann;B. Stieger;M. Stoye;Y. Takahashi;D. Treille;A. Triossi;A. Tsirou;G. I. Veres;N. Wardle;H. K. Wöhri;A. Zagozdzinska;W. D. Zeuner;W. Bertl;K. Deiters;W. Erdmann;R. Horisberger;Q. Ingram;H. C. Kaestli;D. Kotlinski;U. Langenegger;D. Renker;T. Rohe;F. Bachmair;L. Bäni;L. Bianchini;B. Casal;G. Dissertori;M. Dittmar;M. Donegà;P. Eller;C. Grab;C. Heidegger;D. Hits;J. Hoss;G. Kasieczka;W. Lustermann;B. Mangano;M. Marionneau;P. Martinez Ruiz del Arbol;M. Masciovecchio;D. Meister;F. Micheli;P. Musella;F. Nessi-Tedaldi;F. Pandolfi;J. Pata;F. Pauss;L. Perrozzi;M. Quittnat;M. Rossini;A. Starodumov;M. Takahashi;V. R. Tavolaro;K. Theofilatos;R. Wallny;T. K. Aarrestad;C. Amsler;L. Caminada;M. F. Canelli;V. Chiochia;A. De Cosa;C. Galloni;A. Hinzmann;T. Hreus;B. Kilminster;C. Lange;J. Ngadiuba;D. Pinna;P. Robmann;F. J. Ronga;D. Salerno;Y. Yang;M. Cardaci;K. H. Chen;T. H. Doan;Sh. Jain;R. Khurana;M. Konyushikhin;C. M. Kuo;W. Lin;Y. J. Lu;S. S. Yu;Arun Kumar;R. Bartek;P. Chang;Y. H. Chang;Y. Chao;K. F. Chen;P. H. Chen;C. Dietz;F. Fiori;U. Grundler;W. -S. Hou;Y. Hsiung;Y. F. Liu;R. -S. Lu;M. Miñano Moya;E. Petrakou;J. f. Tsai;Y. M. Tzeng;B. Asavapibhop;K. Kovitanggoon;G. Singh;N. Srimanobhas;N. Suwonjandee;A. Adiguzel;M. N. Bakirci;Z. S. Demiroglu;C. Dozen;I. Dumanoglu;E. Eskut;S. Girgis;G. Gokbulut;Y. Guler;Y. Guler;E. Gurpinar;I. Hos;E. E. Kangal;A. Kayis Topaksu;G. Onengut;K. Ozdemir;A. Polatoz;D. Sunar Cerci;M. Vergili;C. Zorbilmez;I. V. Akin;B. Bilin;S. Bilmis;B. Isildak;G. Karapinar;M. Yalvac;M. Zeyrek;A. Albayrak;E. Gülmez;M. Kaya;O. Kaya;T. Yetkin;K. Cankocak;S. Sen;F. I. Vardarlı;B. Grynyov;L. Levchuk;P. Sorokin;R. Aggleton;F. Ball;L. Beck;J. J. Brooke;E. Clement;D. Cussans;H. Flacher;J. Goldstein;M. Grimes;G. P. Heath;H. F. Heath;J. Jacob;L. Kreczko;C. Lucas;Z. Meng;D. M. Newbold;S. Paramesvaran;A. Poll;T. Sakuma;S. Seif El Nasr-storey;S. Senkin;D. Smith;V. J. Smith;K. W. Bell;A. Belyaev;C. Brew;R. M. Brown;D. Cieri;D. J. A. Cockerill;J. A. Coughlan;K. Harder;S. Harper;E. Olaiya;D. Petyt;C. H. Shepherd-Themistocleous;A. Thea;I. R. Tomalin;T. Williams;W. J. Womersley;S. D. Worm;M. Baber;R. Bainbridge;O. Buchmuller;A. 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Joshi;A. W. Jung;B. Klima;B. Kreis;S. Kwan;S. Lammel;J. Linacre;D. Lincoln;R. Lipton;T. Liu;R. Lopes De Sá;J. Lykken;K. Maeshima;J. M. Marraffino;V. I. Martinez Outschoorn;S. Maruyama;D. Mason;P. McBride;P. Merkel;K. Mishra;S. Mrenna;S. Nahn;C. Newman-Holmes;V. O’Dell;K. Pedro;O. Prokofyev;G. Rakness;E. Sexton-Kennedy;A. Soha;W. J. Spalding;L. Spiegel;L. Taylor;S. Tkaczyk;N. V. Tran;L. Uplegger;E. W. Vaandering;C. Vernieri;M. Verzocchi;R. Vidal;H. A. Weber;A. Whitbeck;F. Yang;D. Acosta;P. Avery;P. Bortignon;D. Bourilkov;A. Carnes;M. Carver;D. Curry;S. Das;G. P. Di Giovanni;R. D. Field;I. K. Furic;J. Hugon;J. Konigsberg;A. Korytov;J. F. Low;P. Ma;K. Matchev;H. Mei;P. Milenovic;G. Mitselmakher;D. Rank;R. Rossin;L. Shchutska;M. Snowball;D. Sperka;N. Terentyev;L. Thomas;J. Wang;S. Wang;J. Yelton;S. Hewamanage;S. Linn;P. Markowitz;G. Martinez;J. L. Rodriguez;J. R. Adams;A. Ackert;T. Adams;A. Askew;J. Bochenek;B. Diamond;J. Haas;S. Hagopian;V. Hagopian;K. F. Johnson;A. Khatiwada;H. 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Thomassen;M. Walker;M. Foerster;G. Riley;K. Rose;S. Spanier;A. York;O. Bouhali;A. Castaneda Hernandez;M. Dalchenko;M. De Mattia;A. Delgado;S. Dildick;S. Dildick;R. Eusebi;J. Gilmore;T. Kamon;V. Krutelyov;V. Krutelyov;R. Mueller;I. Osipenkov;Y. Pakhotin;R. Patel;R. Patel;A. Perloff;A. Rose;A. Safonov;A. Tatarinov;K. A. Ulmer;N. Akchurin;C. Cowden;J. Damgov;C. Dragoiu;P. R. Dudero;J. Faulkner;S. Kunori;K. Lamichhane;S. W. Lee;T. Libeiro;S. Undleeb;I. Volobouev;E. Appelt;A. G. Delannoy;S. Greene;A. Gurrola;R. Janjam;W. Johns;C. Maguire;Y. Mao;A. Melo;H. Ni;P. Sheldon;B. Snook;S. Tuo;J. Velkovska;Q. Xu;M. W. Arenton;B. Cox;B. Francis;J. Goodell;R. Hirosky;A. Ledovskoy;H. Li;C. Lin;C. Neu;X. Sun;Y. Wang;E. Wolfe;J. Wood;F. Xia;C. Clarke;R. Harr;P. E. Karchin;C. Kottachchi Kankanamge Don;P. Lamichhane;J. Sturdy;D. A. Belknap;D. Carlsmith;M. Cepeda;S. Dasu;L. Dodd;S. Duric;E. Friis;B. Gomber;M. Grothe;R. Hall-Wilton;M. Herndon;A. Hervé;P. Klabbers;A. Lanaro;A. Levine;K. Long;R. Loveless;A. Mohapatra;I. Ojalvo;T. Perry;G. A. Pierro;G. Polese;T. Ruggles;T. Sarangi;A. Savin;A. Sharma;N. Smith;W. H. Smith;D. Taylor;N. Woods
2016-01-01
Abstract
The cross section for tt¯ production in the all-jets final state is measured in pp collisions at a centre-of-mass energy of 8 TeV at the LHC with the CMS detector, in data corresponding to an integrated luminosity of 18.4 fb−1. The inclusive cross section is found to be 275.6±6.1(stat)±37.8(syst)±7.2(lumi) ,pb. The normalized differential cross sections are measured as a function of the top quark transverse momenta, pT, and compared to predictions from quantum chromodynamics. The results are reported at detector, parton, and particle levels. In all cases, the measured top quark pT spectra are significantly softer than theoretical predictions.
Khachatryan, V.; Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Asilar, E.; Bergauer, T.; Brandstetter, J.; Brondolin, E.; Dragicevic, M.; Erö, J.; Friedl, ...espandi
(2016). Measurement of the tt¯ production cross section in the all-jets final state in pp collisions at √s = 8 TeV [journal article - articolo]. In THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS. Retrieved from http://hdl.handle.net/10446/140522
Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/10446/140522
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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.