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Bhat, MA and Dugad, S and Kumar Verma, R and Sarkar, U and Banerjee, S and Chatterjee, S and Das, P and Guchait, M and Karmakar, S and Kumar, S and Majumder, G and Mazumdar, K and Sahoo, N and Dube, S and Kansal, B and Kapoor, A and Kothekar, K and Pandey, S and Rane, A and Rastogi, A and Bakhshiansohi, H and Chenarani, S and Etesami, SM and Khakzad, M and Mohammadi Najafabadi, M and Naseri, M and Felcini, M and Grunewald, M and Abbrescia, M and Aly, R and Aruta, C and Calabria, C and Colaleo, A and Creanza, D and De Filippis, N and De Palma, M and Di Florio, A and Di Pilato, A and Elmetenawee, W and Fiore, L and Gelmi, A and Iaselli, G and Ince, M and Lezki, S and Maggi, G and Maggi, M and Margjeka, I and Merlin, JA and My, S and Nuzzo, S and Pompili, A and Pugliese, G and Ranieri, A and Selvaggi, G and Silvestris, L and Simone, FM and Venditti, R and Verwilligen, P and Abbiendi, G and Battilana, C and Bonacorsi, D and Borgonovi, L and Braibant-Giacomelli, S and Campanini, R and 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Malberti, M and Malvezzi, S and Menasce, D and Monti, F and Moroni, L and Paganoni, M and Pedrini, D and Ragazzi, S and Tabarelli de Fatis, T and Valsecchi, D and Zuolo, D and Buontempo, S and Cavallo, N and De Iorio, A and Fabozzi, F and Fienga, F and Iorio, AOM and Layer, L and Lista, L and Meola, S and Paolucci, P and Rossi, B and Sciacca, C and Voevodina, E and Azzi, P and Bacchetta, N and Bisello, D and Boletti, A and Bragagnolo, A and Carlin, R and Checchia, P and De Castro Manzano, P and Dorigo, T and Dosselli, U and Gasparini, F and Gasparini, U and Hoh, SY and Margoni, M and Meneguzzo, AT and Presilla, M and Ronchese, P and Rossin, R and Simonetto, F and Strong, G and Tiko, A and Tosi, M and Yarar, H and Zanetti, M and Zotto, P and Zucchetta, A and Braghieri, A and Calzaferri, S and Fiorina, D and Montagna, P and Ratti, SP and Re, V and Ressegotti, M and Riccardi, C and Salvini, P and Vai, I and Vitulo, P and Biasini, M and Bilei, GM and Ciangottini, D and Fanò, L and 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and Cartiglia, N and Cometti, S and Costa, M and Covarelli, R and Demaria, N and Kiani, B and Legger, F and Mariotti, C and Maselli, S and Migliore, E and Monaco, V and Monteil, E and Monteno, M and Obertino, MM and Ortona, G and Pacher, L and Pastrone, N and Pelliccioni, M and Pinna Angioni, GL and Ruspa, M and Salvatico, R and Siviero, F and Sola, V and Solano, A and Soldi, D and Staiano, A and Trocino, D and Belforte, S and Candelise, V and Casarsa, M and Cossutti, F and Da Rold, A and Della Ricca, G and Vazzoler, F and Dogra, S and Huh, C and Kim, B and Kim, DH and Kim, GN and Lee, J and Lee, SW and Moon, CS and Oh, YD and Pak, SI and Sekmen, S and Yang, YC and Kim, H and Moon, DH and Francois, B and Kim, TJ and Park, J and Cho, S and Choi, S and Go, Y and Ha, S and Hong, B and Lee, K and Lee, KS and Lim, J and Park, SK and Roh, Y and Yoo, J and Goh, J and Gurtu, A and Kim, HS and Kim, Y and Almond, J and Bhyun, JH and Choi, J and Jeon, S and Kim, J and Kim, JS and Ko, S and Kwon, H and Lee, H and Lee, S and Nam, K and Oh, BH and Oh, M and Oh, SB and Radburn-Smith, BC and Seo, H and Yang, UK and Yoon, I and Jeon, D and Kim, JH and Ko, B and Lee, JSH and Park, IC and Watson, IJ and Yoo, HD and Choi, Y and Hwang, C and Jeong, Y and Lee, Y and Yu, I and Veckalns, V and Juodagalvis, A and Rinkevicius, A and Tamulaitis, G and Wan Abdullah, WAT and Yusli, MN and Zolkapli, Z and Benitez, JF and Castaneda Hernandez, A and Murillo Quijada, JA and Valencia Palomo, L and Castilla-Valdez, H and De La Cruz-Burelo, E and Heredia-De La Cruz, I and Lopez-Fernandez, R and Sanchez-Hernandez, A and Carrillo Moreno, S and Oropeza Barrera, C and Ramirez-Garcia, M and Vazquez Valencia, F and Eysermans, J and Pedraza, I and Salazar Ibarguen, HA and Uribe Estrada, C and Morelos Pineda, A and Mijuskovic, J and Raicevic, N and Krofcheck, D and Bheesette, S and Butler, PH and Ahmad, A and Asghar, MI and Awan, MIM and Hassan, Q and Hoorani, HR and Khan, WA and Shah, MA and Shoaib, M and 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Smirnov, I and Sosnov, D and Sulimov, V and Uvarov, L and Volkov, S and Vorobyev, A and Andreev, Yu and Dermenev, A and Gninenko, S and Golubev, N and Karneyeu, A and Kirsanov, M and Krasnikov, N and Pashenkov, A and Pivovarov, G and Tlisov, D and Toropin, A and Epshteyn, V and Gavrilov, V and Lychkovskaya, N and Nikitenko, A and Popov, V and Pozdnyakov, I and Safronov, G and Spiridonov, A and Stepennov, A and Toms, M and Vlasov, E and Zhokin, A and Aushev, T and Bychkova, O and Chadeeva, M and Philippov, D and Popova, E and Rusinov, V and Andreev, V and Azarkin, M and Dremin, I and Kirakosyan, M and Terkulov, A and Boos, E and Dubinin, M and Dudko, L and Ershov, A and Gribushin, A and Klyukhin, V and Kodolova, O and Lokhtin, I and Obraztsov, S and Petrushanko, S and Savrin, V and Snigirev, A and Blinov, V and Dimova, T and Kardapoltsev, L and Ovtin, I and Skovpen, Y and Azhgirey, I and Bayshev, I and Kachanov, V and Kalinin, A and Konstantinov, D and Petrov, V and Ryutin, R and Sobol, 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Trembath-Reichert, S and Vetens, W and Collaboration, CMS (2020) Search for resonant pair production of Higgs bosons in the bbZZ channel in proton-proton collisions at s =13 TeV. In: Physical Review D, 102 (3).
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Abstract
A search for the production of a narrow-width resonance decaying into a pair of Higgs bosons decaying into the bbZZ channel is presented. The analysis is based on data collected with the CMS detector during 2016, in proton-proton collisions at the LHC, corresponding to an integrated luminosity of 35.9 fb-1. The final states considered are the ones where one of the Z bosons decays into a pair of muons or electrons, and the other Z boson decays to either a pair of quarks or a pair of neutrinos. Upper limits at 95 confidence level are placed on the production of narrow-width spin-0 or spin-2 particles decaying to a pair of Higgs bosons, in models with and without an extended Higgs sector. For a resonance mass range between 260 and 1000 GeV, limits on the production cross section times branching fraction of a spin-0 and spin-2 resonance range from 0.1 to 5.0 pb and 0.1 to 3.6 pb, respectively. These results set limits in parameter space in bulk Randall-Sundrum radion, Kaluza-Klein excitation of the graviton, and next-to-minimal two-Higgs doublet models (N2HDMs). For specific choices of parameters the N2HDM can be excluded in a mass range between 360 and 620 GeV for a resonance decaying to two Higgs bosons. This is the first search for Higgs boson resonant pair production in the bbZZ channel. © 2020 American Physical Society. All rights reserved.
Item Type: | Journal Article |
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Publication: | Physical Review D |
Publisher: | American Physical Society |
Additional Information: | The copyright for this article belongs to the Author(S). |
Department/Centre: | Division of Interdisciplinary Sciences > Robert Bosch Centre for Cyber Physical Systems Division of Mechanical Sciences > Civil Engineering Division of Physical & Mathematical Sciences > Centre for High Energy Physics |
Date Deposited: | 13 Jan 2023 07:26 |
Last Modified: | 13 Jan 2023 07:26 |
URI: | https://eprints.iisc.ac.in/id/eprint/79117 |
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