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The production of the f1(1285)γf1(1285)γ and a1(1260)γ in colliding e+e-beams in threshold domain

    https://doi.org/10.1142/S0217751X17501238Cited by:3 (Source: Crossref)

    The processes e+e(f1(1285),a1(1260))γ in the threshold domain are considered in the framework of the extended Nambu–Jona-Lasinio model. The channels with the ground ρ(770), ω(782) and radially excited ρ(1450), ω(1420) intermediate meson states are taken into account. It is shown that in the process e+ef1(1285)γ, the probability of the subprocesses with ρ-mesons significantly exceeds the probability of the subprocesses with ω-mesons, whereas, in the process e+ea1(1260)γ, ρ- and ω-channels give approximately equal contributions. The mechanism of this effect is discussed. The radiative decay widths of ρ(1450)f1(1285)γ, ω(1420)f1(1285)γ, ρ(1450)a1(1260)γ and ω(1420)a1(1260)γ are calculated.

    PACS: 12.39.Fe, 13.25.Jx, 13.60.Le, 13.66.Bc, 14.40.Be
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