{"paper":{"title":"Higgs boson decay $h^0\\rightarrow m_VZ$ in the BLMSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guo-Zhu Ning, Hai-Bin Zhang, Jian-Bin Chen, Jing-Jing Feng, Shu-Min Zhao, Tai-Fu Feng","submitted_at":"2018-05-14T08:00:39Z","abstract_excerpt":"In the framework of BLMSSM, the Higgs decays $h^0\\rightarrow Z\\gamma$ and $h^0\\rightarrow m_VZ$ are studied where $m_V$ represents a vector meson($\\rho, \\omega, \\phi, J/\\psi, \\Upsilon$ etc.). Corrections to the CP-even and CP-odd $h^0\\gamma Z$ couplings occur via loop diagrams where new particles are involved. Actually both of them obviously influence the decay rates of $h^0\\rightarrow Z\\gamma$ and $h^0\\rightarrow m_VZ$. Concretely, our obtained numerical result shows that the decay width of $h^0\\rightarrow Z\\gamma$ can be 1.3 times larger than the prediction of the Standard Model(SM). For the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.05048","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}