{ "id": "1810.10056", "version": "v1", "published": "2018-10-23T19:07:52.000Z", "updated": "2018-10-23T19:07:52.000Z", "title": "Search for rare decays of Z and Higgs bosons to J$/ψ$ and a photon in proton-proton collisions at $\\sqrt{s}=$ 13 TeV", "authors": [ "CMS Collaboration" ], "comment": "Submitted to Eur. Phys. J. C. All figures and tables can be found at http://cms-results.web.cern.ch/cms-results/public-results/publications/SMP-17-012 (CMS Public Pages)", "categories": [ "hep-ex" ], "abstract": "A search is presented for decays of Z and Higgs bosons to a J$/\\psi$ meson and a photon, with the subsequent decay of the J$/\\psi$ to $\\mu^+\\mu^-$. The analysis uses data from proton-proton collisions with an integrated luminosity of 35.9 fb$^{-1}$ at $\\sqrt{s}=$ 13 TeV collected with the CMS detector at the LHC. The observed limit on the Z$\\to$J$/\\psi \\gamma$ decay branching fraction, assuming that the J$/\\psi$ meson is produced unpolarized, is 1.4$\\times$10$^{-6}$ at 95% confidence level, which corresponds to a rate higher than expected in the standard model by a factor of 15. For extreme-polarization scenarios, the observed limit changes from -13.6 to +8.6% with respect to the unpolarized scenario. The observed upper limit on the branching fraction for H$\\to$J$/\\psi \\gamma$ where the J$/\\psi$ meson is assumed to be transversely polarized is 7.6$\\times$10$^{-4}$, a factor of 260 larger than the standard model prediction. The results for the Higgs boson are combined with previous data from proton-proton collisions at $\\sqrt{s}=$ 8 TeV to produce an observed upper limit on the branching fraction for H$\\to$J$/\\psi \\gamma$ that is a factor of 220 larger than the standard model value.", "revisions": [ { "version": "v1", "updated": "2018-10-23T19:07:52.000Z" } ], "analyses": { "keywords": [ "proton-proton collisions", "higgs boson", "rare decays", "branching fraction", "upper limit" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }