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IRIS
A search for pairs of dijet resonances with the same mass is conducted in final states with at least four jets. Results are presented separately for the case where the four jet production proceeds via an intermediate resonant state and for nonresonant production. The search uses a data sample corresponding to an integrated luminosity of 138 fb(-1) collected by the CMS detector in proton-proton collisions at root s = 13 TeV. Model-independent limits, at 95% confidence level, are reported on the production cross section of four-jet and dijet resonances. These first LHC limits on resonant pair production of dijet resonances via high mass intermediate states are applied to a signal model of diquarks that decay into pairs of vector-like quarks, excluding diquark masses below 7.6 TeV for a particular model scenario. There are two events in the tails of the distributions, each with a four-jet mass of 8 TeV and an average dijet mass of 2 TeV, resulting in local and global significances of 3.9 and 1.6 standard deviations, respectively, if interpreted as a signal. The nonresonant search excludes pair production of top squarks with masses between 0.50 TeV to 0.77 TeV, with the exception of a small interval between 0.52 and 0.58 TeV, for supersymmetric R-parity-violating decays to quark pairs, significantly extending previous limits. Here, the most significant excess above the predicted background occurs at an average dijet mass of 0.95 TeV, for which the local and global significances are 3.6 and 2.5 standard deviations, respectively.
Search for resonant and nonresonant production of pairs of dijet resonances in proton-proton collisions at sqrt{s} = 13 TeV
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Iashvili;A. Kharchilava;C. McLean;M. Morris;D. Nguyen;J. Pekkanen;S. Rappoccio;A. Williams;G. Alverson;E. Barberis;Y. Haddad;Y. Han;A. Krishna;J. Li;J. Lidrych;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;M. Cremonesi;A. Das;R. Goldouzian;M. Hildreth;K. Hurtado Anampa;C. Jessop;K. Lannon;J. Lawrence;N. Loukas;L. Lutton;J. Mariano;N. Marinelli;I. Mcalister;T. McCauley;C. Mcgrady;K. Mohrman;C. Moore;Y. Musienko;H. Nelson;R. Ruchti;A. Townsend;M. Wayne;H. Yockey;M. Zarucki;L. Zygala;B. Bylsma;M. Carrigan;L. S. Durkin;B. Francis;C. Hill;A. Lesauvage;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;D. Kondratyev;A. M. Koshy;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;D. Acosta;A. Baty;T. Carnahan;M. Decaro;S. Dildick;K. M. Ecklund;P. J. Fern??ndez Manteca;S. Freed;P. Gardner;F. J. M. Geurts;A. Kumar;W. Li;B. P. Padley;R. Redjimi;J. Rotter;W. Shi;S. Yang;E. Yigitbasi;L. Zhang;Y. Zhang;X. Zuo;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;G. P. Van Onsem;K. Goulianos;B. Chiarito;J. P. Chou;Y. Gershtein;E. Halkiadakis;A. Hart;M. Heindl;T. W. Hu;O. Karacheban;I. Laflotte;A. Lath;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;T. Holmes;E. Nibigira;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;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;F. Romeo;P. Sheldon;S. Tuo;J. Velkovska;J. Viinikainen;B. Cardwell;B. Cox;G. Cummings;J. Hakala;R. Hirosky;M. Joyce;A. Ledovskoy;A. Li;C. Neu;C. E. Perez Lara;B. Tannenwald;P. E. Karchin;N. Poudyal;S. Banerjee;K. Black;T. Bose;S. Dasu;I. De Bruyn;P. Everaerts;C. Galloni;H. He;M. Herndon;A. Herve;C. K. Koraka;A. Lanaro;A. Loeliger;R. Loveless;J. Madhusudanan Sreekala;A. Mallampalli;A. Mohammadi;S. Mondal;G. Parida;D. Pinna;A. Savin;V. Shang;V. Sharma;W. H. Smith;D. Teague;H. F. Tsoi;W. Vetens;S. Afanasiev;V. Andreev;Yu. Andreev;T. Aushev;M. Azarkin;A. Babaev;A. Belyaev;V. Blinov;E. Boos;V. Borshch;D. Budkouski;V. Bunichev;O. Bychkova;V. Chekhovsky;R. Chistov;M. Danilov;A. Dermenev;T. Dimova;I. Dremin;M. Dubinin;L. Dudko;V. Epshteyn;A. Ershov;G. Gavrilov;V. Gavrilov;S. Gninenko;V. Golovtcov;N. Golubev;I. Golutvin;I. Gorbunov;A. Gribushin;V. Ivanchenko;Y. Ivanov;V. Kachanov;L. Kardapoltsev;V. Karjavine;A. Karneyeu;V. Kim;M. Kirakosyan;D. Kirpichnikov;M. Kirsanov;V. Klyukhin;O. Kodolova;D. Konstantinov;V. Korenkov;A. Kozyrev;N. Krasnikov;E. Kuznetsova;A. Lanev;P. Levchenko;A. Litomin;N. Lychkovskaya;V. Makarenko;A. Malakhov;V. Matveev;V. Murzin;A. Nikitenko;S. Obraztsov;V. Okhotnikov;A. Oskin;I. Ovtin;V. Palichik;V. Perelygin;M. Perfilov;G. Pivovarov;S. Polikarpov;V. Popov;O. Radchenko;M. Savina;V. Savrin;D. Selivanova;V. Shalaev;S. Shmatov;S. Shulha;Y. Skovpen;S. Slabospitskii;V. Smirnov;D. Sosnov;A. Stepennov;V. Sulimov;E. Tcherniaev;A. Terkulov;O. Teryaev;I. Tlisova;M. Toms;A. Toropin;L. Uvarov;A. Uzunian;E. Vlasov;A. Vorobyev;N. Voytishin;B. S. Yuldashev;A. Zarubin;I. Zhizhin;A. Zhokin
2023-01-01
Abstract
A search for pairs of dijet resonances with the same mass is conducted in final states with at least four jets. Results are presented separately for the case where the four jet production proceeds via an intermediate resonant state and for nonresonant production. The search uses a data sample corresponding to an integrated luminosity of 138 fb(-1) collected by the CMS detector in proton-proton collisions at root s = 13 TeV. Model-independent limits, at 95% confidence level, are reported on the production cross section of four-jet and dijet resonances. These first LHC limits on resonant pair production of dijet resonances via high mass intermediate states are applied to a signal model of diquarks that decay into pairs of vector-like quarks, excluding diquark masses below 7.6 TeV for a particular model scenario. There are two events in the tails of the distributions, each with a four-jet mass of 8 TeV and an average dijet mass of 2 TeV, resulting in local and global significances of 3.9 and 1.6 standard deviations, respectively, if interpreted as a signal. The nonresonant search excludes pair production of top squarks with masses between 0.50 TeV to 0.77 TeV, with the exception of a small interval between 0.52 and 0.58 TeV, for supersymmetric R-parity-violating decays to quark pairs, significantly extending previous limits. Here, the most significant excess above the predicted background occurs at an average dijet mass of 0.95 TeV, for which the local and global significances are 3.6 and 2.5 standard deviations, respectively.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11563/174294
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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.