A search is presented for narrow heavy resonances X decaying into pairs of Higgs bosons (H) in proton-proton collisions collected by the CMS experiment at the LHC at root s = 8 TeV. The data correspond to an integrated luminosity of 19.7 fb(-1). The search considers HH resonances with masses between 1 and 3 TeV, having final states of two b quark pairs. Each Higgs boson is produced with large momentum, and the hadronization products of the pair of b quarks can usually be reconstructed as single large jets. The background from multijet and t (t) over bar events is significantly reduced by applying requirements related to the flavor of the jet, its mass, and its substructure. The signal would be identified as a peak on top of the dijet invariant mass spectrum of the remaining background events. No evidence is observed for such a signal. Upper limits obtained at 95 confidence level for the product of the production cross section and branching fraction sigma(gg -> X) B(X -> HH -> b (b) over barb (b) over bar) range from 10 to 1.5 fb for the mass of X from 1.15 to 2.0 TeV, significantly extending previous searches. For a warped extra dimension theory with amass scale Lambda(R) = 1 TeV, the data exclude radion scalar masses between 1.15 and 1.55 TeV.
Search for heavy resonances decaying to two Higgs bosons in final states containing four b quarks / Khachatryan, V; Sirunyan, Am; Tumasyan, A; Adam, W; Asilar, E; Bergauer, T; Brandstetter, J; Brondolin, E; Dragicevic, M; Erö, J; Flechl, M; Friedl, M; Frühwirth, R; Ghete, Vm; Hartl, C; Hörmann, N; Hrubec, J; Jeitler, M; König, A; Krammer, M; Krätschmer, I; Liko, D; Matsushita, T; Mikulec, I; Rabady, D; Rad, N; Rahbaran, B; Rohringer, H; Schieck, J; Schöfbeck, R; Strauss, J; Treberer-Treberspurg, W; Waltenberger, W; Wulz, Ce; Mossolov, V; Shumeiko, N; Suarez Gonzalez, J; Alderweireldt, S; Cornelis, T; De Wolf, Ea; Janssen, X; Knutsson, A; Lauwers, J; Luyckx, S; Van De Klundert, M; Van Haevermaet, H; Van Mechelen, P; Van Remortel, N; Van Spilbeeck, A; Abu Zeid, S; Blekman, F; D'Hondt, J; Daci, N; De Bruyn, I; Deroover, K; Heracleous, N; Keaveney, J; Lowette, S; Moortgat, S; Moreels, L; Olbrechts, A; Python, Q; Strom, D; Tavernier, S; Van Doninck, W; Van Mulders, P; Van Onsem, Gp; Van Parijs, I; 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Woods, N. - In: THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS. - ISSN 1434-6044. - STAMPA. - 76:7(2016). [10.1140/epjc/s10052-016-4206-6]
Search for heavy resonances decaying to two Higgs bosons in final states containing four b quarks
Khachatryan V; Sirunyan AM; Tumasyan A; Adam W; Asilar E; Bergauer T; Brandstetter J; Brondolin E; Dragicevic M; Erö J; Flechl M; Friedl M; Frühwirth R; Ghete VM; Hartl C; Hörmann N; Hrubec J; Jeitler M; König A; Krammer M; Krätschmer I; Liko D; Matsushita T; Mikulec I; Rabady D; Rad N; Rahbaran B; Rohringer H; Schieck J; Schöfbeck R; Strauss J; Treberer-Treberspurg W; Waltenberger W; Wulz CE; Mossolov V; Shumeiko N; Suarez Gonzalez J; Alderweireldt S; Cornelis T; De Wolf EA; Janssen X; Knutsson A; Lauwers J; Luyckx S; Van De Klundert M; Van Haevermaet H; Van Mechelen P; Van Remortel N; Van Spilbeeck A; Abu Zeid S; Blekman F; D'Hondt J; Daci N; De Bruyn I; Deroover K; Heracleous N; Keaveney J; Lowette S; Moortgat S; Moreels L; Olbrechts A; Python Q; Strom D; Tavernier S; Van Doninck W; Van Mulders P; Van Onsem GP; Van Parijs I; Barria P; Brun H; Caillol C; Clerbaux B; De Lentdecker G; Fasanella G; Favart L; Goldouzian R; Grebenyuk A; Karapostoli G; Lenzi T; Léonard A; Maerschalk T; Marinov A; Perniè L; Randle-Conde A; Seva T; Vander Velde C; Vanlaer P; Yonamine R; Zenoni F; Zhang F; Beernaert K; Benucci L; Cimmino A; Crucy S; Dobur D; Fagot A; Garcia G; Gul M; Mccartin J; Ocampo Rios AA; Poyraz D; Ryckbosch D; Salva S; Sigamani M; Tytgat M; Van Driessche W; Yazgan E; Zaganidis N; Basegmez S; Beluffi C; Bondu O; Brochet S; Bruno G; Caudron A; Ceard L; Visscher S; Delaere C; Delcourt M; Favart D; Forthomme L; Giammanco A; Jafari A; Jez P; Komm M; Lemaitre V; Mertens A; Musich M; Nuttens C; Perrini L; Piotrzkowski K; Popov A; Quertenmont L; Selvaggi M; Vidal Marono M; Beliy N; Hammad GH; Aldá Júnior WL; Alves FL; Alves GA; Brito L; Correa Martins Junior M; Hamer M; Hensel C; Moraes A; Pol ME; Rebello Teles P; Belchior Batista Das Chagas E; Carvalho W; Chinellato J; Custódio A; Da Costa EM; De Jesus Damiao D; De Oliveira Martins C; Fonseca De Souza S; Huertas Guativa LM; Malbouisson H; Matos Figueiredo D; Mora Herrera C; Mundim L; Nogima H; Prado Da Silva WL; Santoro A; Sznajder A; Tonelli Manganote EJ; Vilela Pereira A; Ahuja S; Bernardes CA; De Souza Santos A; Dogra S; Fernandez Perez Tomei TR; Gregores EM; Mercadante PG; Moon CS; Novaes SF; Padula SS; Romero Abad D; Ruiz Vargas JC; Aleksandrov A; Hadjiiska R; Iaydjiev P; Rodozov M; Stoykova S; Sultanov G; Vutova M; Dimitrov A; Glushkov I; Litov L; Pavlov B; Petkov P; Fang W; Ahmad M; Bian JG; Chen GM; Chen HS; Chen M; Cheng T; Du R; Jiang CH; Leggat D; Plestina R; Romeo F; Shaheen SM; Spiezia A; Tao J; Wang C; Wang Z; Zhang H; Asawatangtrakuldee C; Ban Y; Li Q; Liu S; Mao Y; Qian SJ; Wang D; Xu Z; Avila C; Cabrera A; Chaparro Sierra LF; Florez C; Gomez JP; Gomez Moreno B; Sanabria JC; Godinovic N; Lelas D; Puljak I; Ribeiro Cipriano PM; Antunovic Z; Kovac M; Brigljevic V; Kadija K; Luetic J; Micanovic S; Sudic L; Attikis A; Mavromanolakis G; Mousa J; Nicolaou C; Ptochos F; Razis PA; Rykaczewski H; Finger M; Finger M Jr; Assran Y; Ellithi Kamel A; Mahrous A; Radi A; Calpas B; Kadastik M; Murumaa M; Raidal M; Tiko A; 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2016-01-01
Abstract
A search is presented for narrow heavy resonances X decaying into pairs of Higgs bosons (H) in proton-proton collisions collected by the CMS experiment at the LHC at root s = 8 TeV. The data correspond to an integrated luminosity of 19.7 fb(-1). The search considers HH resonances with masses between 1 and 3 TeV, having final states of two b quark pairs. Each Higgs boson is produced with large momentum, and the hadronization products of the pair of b quarks can usually be reconstructed as single large jets. The background from multijet and t (t) over bar events is significantly reduced by applying requirements related to the flavor of the jet, its mass, and its substructure. The signal would be identified as a peak on top of the dijet invariant mass spectrum of the remaining background events. No evidence is observed for such a signal. Upper limits obtained at 95 confidence level for the product of the production cross section and branching fraction sigma(gg -> X) B(X -> HH -> b (b) over barb (b) over bar) range from 10 to 1.5 fb for the mass of X from 1.15 to 2.0 TeV, significantly extending previous searches. For a warped extra dimension theory with amass scale Lambda(R) = 1 TeV, the data exclude radion scalar masses between 1.15 and 1.55 TeV.
Citazione
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C, PARTICLES AND FIELDS. - ISSN 1434-6044. - STAMPA. - 76:7(2016). [10.1140/epjc/s10052-016-4206-6]
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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.