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Main Author: Rashed, Ahmed
Format: Preprint
Published: 2024
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Online Access:https://arxiv.org/abs/2412.09926
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author Rashed, Ahmed
author_facet Rashed, Ahmed
contents We investigate the decay process $J/ψ\rightarrow e^+ e^-ϕ$, where the relatively clean electromagnetic (EM) transitions dominate at leading order at the tree level, while hadronic contributions arise only through hadronic loop transitions. The branching ratio of $J/ψ\rightarrow e^+ e^-ϕ$ was estimated to be approximately $2.28 \times 10^{-8}$ keV where the hadronic effects are negligible compared to the EM contributions. The upper limit on the branching fraction was set to be $B(J/ψ\rightarrow e^+ e^-ϕ) < 1.2 \times 10^{-7}$ by BESIII collaboration. In this paper we investigate the existence of a neutral state such as dark photon and dark $Z$. Our analysis shows that the constraints on the dark photon and dark $Z$ are stringent in the way that large enhancement to the SM branching ratio up to the present experimental limit is not possible. Therefore, observing a signal for the dark photon and dark $Z$ in this decay channel is changeable.
format Preprint
id arxiv_https___arxiv_org_abs_2412_09926
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Searching for neutral state in the rare decay $J/ψ\rightarrow e^+ e^- ϕ$
Rashed, Ahmed
High Energy Physics - Phenomenology
We investigate the decay process $J/ψ\rightarrow e^+ e^-ϕ$, where the relatively clean electromagnetic (EM) transitions dominate at leading order at the tree level, while hadronic contributions arise only through hadronic loop transitions. The branching ratio of $J/ψ\rightarrow e^+ e^-ϕ$ was estimated to be approximately $2.28 \times 10^{-8}$ keV where the hadronic effects are negligible compared to the EM contributions. The upper limit on the branching fraction was set to be $B(J/ψ\rightarrow e^+ e^-ϕ) < 1.2 \times 10^{-7}$ by BESIII collaboration. In this paper we investigate the existence of a neutral state such as dark photon and dark $Z$. Our analysis shows that the constraints on the dark photon and dark $Z$ are stringent in the way that large enhancement to the SM branching ratio up to the present experimental limit is not possible. Therefore, observing a signal for the dark photon and dark $Z$ in this decay channel is changeable.
title Searching for neutral state in the rare decay $J/ψ\rightarrow e^+ e^- ϕ$
topic High Energy Physics - Phenomenology
url https://arxiv.org/abs/2412.09926