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Search for Higgs and Z boson decays to J/ψ or Y pairs in the four-muon final state in proton-proton collisions at √s = 13 TeV

Sirunyan, AM and Tumasyan, A and Adam, W and Ambrogi, F and Bergauer, T and Brandstetter, J and Dragicevic, M and Erö, J and Escalante Del Valle, A and Flechl, M and Frühwirth, R and Jeitler, M and Krammer, N and Krätschmer, I and Liko, D and Madlener, T and Mikulec, I and Rad, N and Schieck, J and Schöfbeck, R and Spanring, M and Spitzbart, D and Waltenberger, W and Wulz, C-E and Zarucki, M and Drugakov, V and Mossolov, V and Suarez Gonzalez, J and Darwish, MR and De Wolf, EA and Di Croce, D and Janssen, X and Lauwers, J and Lelek, A and Pieters, M and Rejeb Sfar, H and Van Haevermaet, H and Van Mechelen, P and Van Putte, S and Van Remortel, N and Blekman, F and Bols, ES and Chhibra, SS and D'Hondt, J and De Clercq, J and Lontkovskyi, D and Lowette, S and Marchesini, I and Moortgat, S and Moreels, L and Python, Q and Skovpen, K and Tavernier, S and Van Doninck, W and Van Mulders, P and Van Parijs, I and Beghin, D and Bilin, B and Brun, H and Clerbaux, B and De Lentdecker, G and 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and Karimäki, V and Kinnunen, R and Lampén, T and Lassila-Perini, K and Laurila, S and Lehti, S and Lindén, T and Luukka, P and Mäenpää, T and Siikonen, H and Tuominen, E and Tuominiemi, J and Tuuva, T and Besancon, M and Couderc, F and Dejardin, M and Denegri, D and Fabbro, B and Faure, JL and Ferri, F and Ganjour, S and Givernaud, A and Gras, P and Hamel de Monchenault, G and Jarry, P and Leloup, C and Locci, E and Malcles, J and Rander, J and Rosowsky, A and Sahin, MÃ� and Savoy-Navarro, A and Titov, M and Amendola, C and Beaudette, F and Busson, P and Charlot, C and Diab, B and Falmagne, G and Granier de Cassagnac, R and Kucher, I and Lobanov, A and Martin Perez, C and Nguyen, M and Ochando, C and Paganini, P and Rembser, J and Salerno, R and Sauvan, JB and Sirois, Y and Zabi, A and Zghiche, A and Agram, J-L and Andrea, J and Bloch, D and Bourgatte, G and Brom, J-M and Chabert, EC and Collard, C and Conte, E and Fontaine, J-C and Gelé, D and Goerlach, U and Jansová, M and Le Bihan, 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Sawant, S and Dube, S and Hegde, V and Kapoor, A and Kothekar, K and Pandey, S and Rane, A and Rastogi, A and Chenarani, S and Eskandari Tadavani, E and Etesami, SM and Khakzad, M and Mohammadi Najafabadi, M and Naseri, M and Rezaei Hosseinabadi, F and Felcini, M and Grunewald, M and Abbrescia, M and Calabria, C and Colaleo, A and Creanza, D and Cristella, L and De Filippis, N and De Palma, M and Di Florio, A and Fiore, L and Gelmi, A and Iaselli, G and Ince, M and Lezki, S and Maggi, G and Maggi, M and Miniello, G and My, S and Nuzzo, S and Pompili, A and Pugliese, G and Radogna, R and Ranieri, A and Selvaggi, G and Silvestris, L 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 Capiluppi, P and Castro, A and Cavallo, FR and Ciocca, C and Codispoti, G and Cuffiani, M and Dallavalle, GM and Fabbri, F and Fanfani, A and Fontanesi, E and Giacomelli, P and Grandi, C and Guiducci, L and 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In: Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics, 797 .

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Official URL: https://doi.org/10.1016/j.physletb.2019.134811

Abstract

A search for decays of the Higgs and Z boson to pairs of J/ψ or Y(nS) (n = 1, 2, 3) mesons, with their subsequent decay to μ+μ− pairs, is presented. The analysis uses data from proton-proton collisions at s=13TeV, collected with the CMS detector at the LHC in 2017 and corresponding to an integrated luminosity of 37.5fb−1. While an observation of such a decay with this sample would indicate the presence of physics beyond the standard model, no significant excess is observed. Upper limits at 95% confidence level are placed on the branching fractions of these decays. In the J/ψ pair channel, the limits are 1.8×10−3 and 2.2×10−6 for the Higgs and Z boson, respectively, while in the combined Y(nS) pair channel, the limits are 1.4×10−3 and 1.5×10−6, respectively, when the mesons from the Higgs and Z boson decay are assumed to be unpolarized. When fully longitudinal and transverse polarizations are considered the limits reduce by about 22–29% and increase by about 10–13%, respectively.

Item Type: Journal Article
Publication: Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
Publisher: Elsevier B.V.
Additional Information: The copyright for this article belongs to the Authors.
Keywords: CMS; Higgs boson; Rare decays; Standard model physics; Z boson
Department/Centre: Division of Physical & Mathematical Sciences > Centre for High Energy Physics
Date Deposited: 19 Oct 2022 09:07
Last Modified: 19 Oct 2022 09:07
URI: https://eprints.iisc.ac.in/id/eprint/77341

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