We explore the consequences of treating the X(3872) meson as a tetraquark bound state. As dynamical framework we employ a relativistic constituent quark model which includes infrared confinement in an effective way. We calculate the decay widths of the observed channels X → J/ψ + 2π(3π) and X →D 0 + D 0 + π 0 via the intermediate off-shell states X → J/ψ + ρ(ω) and X →D + D * . For reasonable values of the size parameter ΛX of the X(3872) we find consistency with the available experimental data. We also discuss the possible impact of the X(3872) in a s-channel dominance description of the J/ψ dissociation cross section.
We further explore the consequences of treating the X(3872) meson as a tetraquark bound state by analyzing its one-photon decay X → γ +J/ψ in the framework of our approach developed in previous papers which incorporates quark confinement in an effective way. To introduce electromagnetism we gauge a nonlocal effective Lagrangian describing the interaction of the X(3872) meson with its four constituent quarks by using the P-exponential path-independent formalism. We calculate the matrix element of the transition X → γ + J/ψ and prove its gauge invariance. We evaluate the X → γ + J/ψ decay width and the longitudinal/transverse composition of the J/ψ in this decay. For a reasonable value of the size parameter of the X(3872) meson we find consistency with the available experimental data. We also calculate the helicity and multipole amplitudes of the process, and describe how they can be obtained from the covariant transition amplitude by covariant projection.
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