首页> 外文期刊>International Journal of Modern Physics, A. Particles and Fields, Gravitation, Cosmology >The production of the f(1)(1285)gamma and a(1)(1260)gamma in colliding e(+) e(-)-beams in threshold domain
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The production of the f(1)(1285)gamma and a(1)(1260)gamma in colliding e(+) e(-)-beams in threshold domain

机译:在阈值结构域中碰撞E(+)E( - )梁的F(1)(1285)γ(1260)γ和(1)(1260)γ的生产

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摘要

The processes e(+) e(-) -> (f(1)(1285), a(1)(1260))gamma in the threshold domain are considered in the framework of the extended Nambu-Jona-Lasinio model. The channels with the ground rho(770), omega(782) and radially excited rho(1450), omega(1420) intermediate meson states are taken into account. It is shown that in the process e+ e- -> f(1)(1285)gamma , the probability of the subprocesses with w-mesons significantly exceeds the probability of the subprocesses with w-mesons, whereas, in the process e(+) e(-) -> a(1)(1260)gamma, rho- and w-channels give approximately equal contributions. The mechanism of this effect is discussed. The radiative decay widths of rho(1450) -> f(1)(1285)gamma, omega(1420) -> f(1)(1285)gamma, rho(1450) -> a(1)(1260)gamma and omega(1420) -> a(1)(1260)gamma are calculated.
机译:在延伸的Nambu-jona-Lasinio模型的框架中考虑阈值结构域中的方法E(+)e( - ) - >(f(1)(1285),a(1)(1260))伽马。 考虑到具有地rhO(770),Omega(782)和径向激发的rho(1450),ω(1420)中间介质状态的通道。 结果表明,在过程E + E- - > F(1)(1285)伽马中,具有W-MESONS的子过程的概率显着超过了具有W-MESONS的子过程的概率,而在过程E中(+ )E( - ) - > a(1)(1260)伽玛,rho-和W频道给出了大约相同的贡献。 讨论了这种效果的机制。 Rho(1450) - > F(1)(1285)γ,Omega(1420) - > F(1)(1285)γ,rhO(1450) - > a(1)(1260)γ和 欧米茄(1420) - > A(1)(1260)伽玛。

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