Strong and Electromagnetic Decays of X(1835) as a Baryonium State

dc.creatorMa, Yong-Liang
dc.date2008-08-27
dc.date2009-04-09
dc.date.accessioned2026-07-07T13:04:39Z
dc.date.available2026-07-07T13:04:39Z
dc.descriptionWith the assumption that the recently observed X(1835) is a baryonium state we have studied the strong decays of $X(1835) \to η^{(\prime)} π^+ π^-, η^{(\prime)} π^0 π^0$ and the electromagnetic decay of $X(1835) \to 2γ$ in the framework of effective Lagrangian formalism. In the present investigation we have included the contributions from the iso-singlet light scalar resonances but we have not included the isospin violating effect. Our result for the strong decay of $X(1835) \to η^{\prime} π^+ π^-$ is smaller than the observed data. The decay width for the radiative decay of $X(1835) \to 2γ$ is consistent with the assumption that it decays through the glueball. In addition, the width for the strong decay of $X(1835) \to ηπ^+ π^-$ is larger than that of the strong decay of $X(1835) \to η^{\prime} π^+ π^-$ due to the large phase space and coupling constant $g_{N\bar{N}η}$. From our investigation, it is not possible to interpret X(1835) as a baryonium.
dc.descriptionCorrected typos
dc.identifierhttps://arxiv.org/abs/0808.3764
dc.identifierhttp://arxiv.org/abs/0808.3764
dc.identifierJ.Phys.G36:055004,2009
dc.identifierdoi:10.1088/0954-3899/36/5/055004
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/227236
dc.subjectHigh Energy Physics - Phenomenology
dc.titleStrong and Electromagnetic Decays of X(1835) as a Baryonium State
dc.typetext

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