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CRIS Current Research Information System
A search is reported for massive resonances decaying into a quark and a vector
boson (W or Z), or two vector bosons (WW, WZ, or ZZ). The analysis is performed on an
inclusive sample of multijet events corresponding to an integrated luminosity of 19.7 fb−1,
collected in proton-proton collisions at a centre-of-mass energy of 8TeV with the CMS
detector at the LHC. The search uses novel jet-substructure identification techniques that
provide sensitivity to the presence of highly boosted vector bosons decaying into a pair
of quarks. Exclusion limits are set at a confidence level of 95% on the production of:
(i) excited quark resonances q decaying to qW and qZ for masses less than 3.2TeV and
2.9TeV, respectively, (ii) a Randall-Sundrum graviton GRS decaying into WW for masses
below 1.2TeV, and (iii) a heavy partner of the W boson W
0
decaying into WZ for masses
less than 1.7TeV. For the first time mass limits are set on W
0
! WZ and GRS ! WW in
the all-jets final state. The mass limits on q ! qW, q ! qZ, W
0
! WZ, GRS ! WW
are the most stringent to date. A model with a “bulk” graviton Gbulk that decays into
WW or ZZ bosons is also studied.
S Chatrchyan, V Khachatryan, A M Sirunyan, A Tumasyan,
W Adam, T Bergauer, et al. (2014). Search for massive resonances in dijet systems
containing jets tagged as W or Z boson decays in pp
collisions at
sqrt(s) = 8 TeV. JOURNAL OF HIGH ENERGY PHYSICS, 1408, 173-1-173-36 [10.1007/JHEP08(2014)173].
Search for massive resonances in dijet systems
containing jets tagged as W or Z boson decays in pp
collisions at
sqrt(s) = 8 TeV
S. Chatrchyan;V. Khachatryan;A. M. Sirunyan;A. Tumasyan;W. Adam;T. Bergauer;M. Dragicevic;J. Erö;C. Fabjan;M. Friedl;R. Frühwirth;V. M. Ghete;C. Hartl;N. Hörmann;J. Hrubec;M. Jeitler;W. Kiesenhofer;V. Knünz;M. Krammer;I. Krätschmer;D. Liko;I. Mikulec;D. Rabady;B. Rahbaran;H. Rohringer;R. Schöfbeck;J. Strauss;A. Taurok;W. Treberer Treberspurg;W. Waltenberger;C. E. Wulz;V. Mossolov;N. Shumeiko;J. Suarez Gonzalez;S. Alderweireldt;M. Bansal;S. Bansal;T. Cornelis;E. A. De Wolf;X. Janssen;A. Knutsson;S. Luyckx;S. Ochesanu;B. Roland;R. Rougny;H. Van Haevermaet;P. Van Mechelen;N. Van Remortel;A. Van Spilbeeck;F. Blekman;S. Blyweert;J. D’Hondt;N. Heracleous;A. Kalogeropoulos;J. Keaveney;T. J. Kim;S. Lowette;M. Maes;A. Olbrechts;D. Strom;S. Tavernier;W. Van Doninck;P. Van Mulders;G. P. Van Onsem;I. Villella;C. Caillol;B. Clerbaux;G. De Lentdecker;L. Favart;A. P. R. Gay;A. Léonard;P. E. Marage;A. Mohammadi;L. Perniè;T. Reis;T. Seva;L. Thomas;C. Vander Velde;P. Vanlaer;J. Wang;V. Adler;K. Beernaert;L. Benucci;A. Cimmino;S. Costantini;S. Crucy;S. Dildick;G. Garcia;B. Klein;J. Lellouch;J. Mccartin;A. A. Ocampo Rios;D. Ryckbosch;S. Salva Diblen;M. Sigamani;N. Strobbe;F. Thyssen;M. Tytgat;S. Walsh;E. Yazgan;N. Zaganidis;S. Basegmez;C. Beluffi;G. Bruno;R. Castello;A. Caudron;L. Ceard;G. G. Da Silveira;C. Delaere;T. du Pree;D. Favart;L. Forthomme;A. Giammanco;J. Hollar;P. Jez;M. Komm;V. Lemaitre;J. Liao;O. Militaru;C. Nuttens;D. Pagano;A. Pin;K. Piotrzkowski;A. Popov;L. Quertenmont;M. Selvaggi;M. Vidal Marono;J. M. Vizan Garcia;N. Beliy;T. Caebergs;E. Daubie;G. H. Hammad;G. A. Alves;M. Correa Martins Junior;T. Dos Reis Martins;M. E. Pol;M. H. G. Souza;W. L. Aldá Júnior;W. Carvalho;J. Chinellato;A. Custódio;E. M. Da Costa;D. De Jesus Damiao;C. De Oliveira Martins;S. Fonseca De Souza;H. Malbouisson;M. Malek;D. Matos Figueiredo;L. Mundim;H. Nogima;W. L. Prado Da Silva;J. Santaolalla;A. Santoro;A. Sznajder;E. J. Tonelli Manganote;A. Vilela Pereira;C. A. Bernardesb;F. A. Diasa;T. R. Fernandez Perez Tomeia;E. M. Gregoresb;P. G. Mercadanteb;S. F. Novaesa;Sandra S. Padula;V. Genchev;P. Iaydjiev;A. Marinov;S. Piperov;M. Rodozov;G. Sultanov;M. Vutova;A. Dimitrov;I. Glushkov;R. Hadjiiska;V. Kozhuharov;L. Litov;B. Pavlov;P. Petkov;J. G. Bian;G. M. Chen;H. S. Chen;M. Chen;R. Du;C. H. Jiang;D. Liang;S. Liang;X. Meng;R. Plestina8;J. Tao;X. Wang;Z. Wang;C. Asawatangtrakuldee;Y. Ban;Y. Guo;Q. Li;W. Li;S. Liu;Y. Mao;S. J. Qian;D. Wang;L. Zhang;W. Zou;C. Avila;L. F. Chaparro Sierra;C. Florez;J. P. Gomez;B. Gomez Moreno;J. C. Sanabria;N. Godinovic;D. Lelas;D. Polic;I. Puljak;Z. Antunovic;M. Kovac;V. Brigljevic;K. Kadija;J. Luetic;D. Mekterovic;S. Morovic;L. Sudic;A. Attikis;G. Mavromanolakis;J. Mousa;C. Nicolaou;F. Ptochos;P. A. Razis;M. Finger;M. Finger Jr;Y. Assran;S. Elgammal;A. Ellithi Kamel;M. A. Mahmoud;A. Mahrous;A. Radi;M. Kadastik;M. Müntel;M. Murumaa;M. Raidal;A. Tiko;P. Eerola;G. Fedi;M. Voutilainen;J. Härkönen;V. Karimäki;R. Kinnunen;M. J. Kortelainen;T. 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Dorland;G. Eckerlin;D. Eckstein;T. Eichhorn;G. Flucke;A. Geiser;A. Grebenyuk;P. Gunnellini;S. Habib;J. Hauk;G. Hellwig;M. Hempel;D. Horton;H. Jung;M. Kasemann;P. Katsas;J. Kieseler;C. Kleinwort;M. Krämer;D. Krücker;W. Lange;J. Leonard;K. Lipka;W. Lohmann;B. Lutz;R. Mankel;I. Marfin;I. A. Melzer Pellmann;A. B. Meyer;J. Mnich;A. Mussgiller;S. Naumann Emme;O. Novgorodova;F. Nowak;E. Ntomari;H. Perrey;A. Petrukhin;D. Pitzl;R. Placakyte;A. Raspereza;P. M. Ribeiro Cipriano;C. Riedl;E. Ron;M. Ö. Sahin;J. Salfeld Nebgen;P. Saxena;R. Schmidt;T. Schoerner Sadenius;M. Schröder;M. Stein;A. D. R. Vargas Trevino;R. Walsh;C. Wissing;M. Aldaya Martin;V. Blobel;H. Enderle;J. Erfle;E. Garutti;K. Goebel;M. Görner;M. Gosselink;J. Haller;R. S. Höing;H. Kirschenmann;R. Klanner;R. Kogler;J. Lange;T. Lapsien;T. Lenz;I. Marchesini;J. Ott;T. Peiffer;N. Pietsch;D. Rathjens;C. Sander;H. Schettler;P. Schleper;E. Schlieckau;A. Schmidt;M. Seidel;J. Sibille;V. Sola;H. Stadie;G. Steinbrück;D. Troendle;E. Usai;L. 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Bianchi;P. Bloch;A. Bocci;A. Bonato;O. Bondu;C. Botta;H. Breuker;T. Camporesi;G. Cerminara;T. Christiansen;J. A. Coarasa Perez;S. Colafranceschi;M. D’Alfonso;D. d’Enterria;A. Dabrowski;A. David;F. De Guio;A. De Roeck;S. De Visscher;M. Dobson;N. Dupont Sagorin;A. Elliott Peisert;J. Eugster;G. Franzoni;W. Funk;M. Giffels;D. Gigi;K. Gill;D. Giordano;M. Girone;M. Giunta;F. Glege;R. Gomez Reino Garrido;S. Gowdy;R. Guida;J. Hammer;M. Hansen;P. Harris;J. Hegeman;V. Innocente;P. Janot;E. Karavakis;K. Kousouris;K. Krajczar;P. Lecoq;C. Lourenço;N. Magini;L. Malgeri;M. Mannelli;L. Masetti;F. Meijers;S. Mersi;E. Meschi;F. Moortgat;M. Mulders;P. Musella;L. Orsini;E. Palencia Cortezon;L. Pape;E. Perez;L. Perrozzi;A. Petrilli;G. Petrucciani;A. Pfeiffer;M. Pierini;M. Pimiä;D. Piparo;M. Plagge;A. Racz;W. Reece;G. Rolandi;M. Rovere;H. Sakulin;F. Santanastasio;C. Schäfer;C. Schwick;S. Sekmen;A. Sharma;P. Siegrist;P. Silva;M. Simon;P. Sphicas;D. Spiga;J. Steggemann;B. Stieger;M. Stoye;D. Treille;A. 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Malik;F. Meier;G. R. Snow;J. Dolen;A. Godshalk;I. Iashvili;S. Jain;A. Kharchilava;A. Kumar;S. Rappoccio;G. Alverson;E. Barberis;D. Baumgartel;M. Chasco;J. Haley;A. Massironi;D. Nash;T. Orimoto;D. Trocino;D. Wood;J. Zhang;A. Anastassov;K. A. Hahn;A. Kubik;L. Lusito;N. Mucia;N. Odell;B. Pollack;A. Pozdnyakov;M. Schmitt;S. Stoynev;K. Sung;M. Velasco;S. Won;D. Berry;A. Brinkerhoff;K. M. Chan;A. Drozdetskiy;M. Hildreth;C. Jessop;D. J. Karmgard;N. Kellams;J. Kolb;K. Lannon;W. Luo;S. Lynch;N. Marinelli;D. M. Morse;T. Pearson;M. Planer;R. Ruchti;J. Slaunwhite;N. Valls;M. Wayne;M. Wolf;A. Woodard;L. Antonelli;B. Bylsma;L. S. Durkin;S. Flowers;C. Hill;R. Hughes;K. Kotov;T. Y. Ling;D. Puigh;M. Rodenburg;G. Smith;C. Vuosalo;B. L. Winer;H. Wolfe;H. W. Wulsin;E. Berry;P. Elmer;V. Halyo;P. Hebda;A. Hunt;P. Jindal;S. A. Koay;P. Lujan;D. Marlow;T. Medvedeva;M. Mooney;J. Olsen;P. Piroué;X. Quan;A. Raval;H. Saka;D. Stickland;C. Tully;J. S. Werner;S. C. Zenz;A. Zuranski;E. Brownson;A. Lopez;H. Mendez;J. 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2014
Abstract
A search is reported for massive resonances decaying into a quark and a vector
boson (W or Z), or two vector bosons (WW, WZ, or ZZ). The analysis is performed on an
inclusive sample of multijet events corresponding to an integrated luminosity of 19.7 fb−1,
collected in proton-proton collisions at a centre-of-mass energy of 8TeV with the CMS
detector at the LHC. The search uses novel jet-substructure identification techniques that
provide sensitivity to the presence of highly boosted vector bosons decaying into a pair
of quarks. Exclusion limits are set at a confidence level of 95% on the production of:
(i) excited quark resonances q decaying to qW and qZ for masses less than 3.2TeV and
2.9TeV, respectively, (ii) a Randall-Sundrum graviton GRS decaying into WW for masses
below 1.2TeV, and (iii) a heavy partner of the W boson W
0
decaying into WZ for masses
less than 1.7TeV. For the first time mass limits are set on W
0
! WZ and GRS ! WW in
the all-jets final state. The mass limits on q ! qW, q ! qZ, W
0
! WZ, GRS ! WW
are the most stringent to date. A model with a “bulk” graviton Gbulk that decays into
WW or ZZ bosons is also studied.
S Chatrchyan, V Khachatryan, A M Sirunyan, A Tumasyan,
W Adam, T Bergauer, et al. (2014). Search for massive resonances in dijet systems
containing jets tagged as W or Z boson decays in pp
collisions at
sqrt(s) = 8 TeV. JOURNAL OF HIGH ENERGY PHYSICS, 1408, 173-1-173-36 [10.1007/JHEP08(2014)173].
S Chatrchyan; V Khachatryan; A M Sirunyan; A Tumasyan;
W Adam; T Bergauer; M Dragicevic; J Erö; C Fabjan; M Friedl; R Frühwirth; V M Ghete; C Hartl; ...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/416974
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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.