2002理论物理通讯:英文版Requires access

Baryon + Baryon→(ΩΩ)J^π=0+ + X Cross Section Calculation

YUYou-Wen

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Abstract

The cross sections ofΩ + Ξ→ (ΩΩ)Jπ=0+ + K(K*) and Ω + Ω→ (ΩΩ)Jπ 0+ + η(φ) are studied by using an effective Hamiltonian method.For the two pseudo-scalar meson production processes,the cross sections are still in the order of severalμbs,but for the two vector meson production processes,the cross sections are about 10 times larger than those in pseudo-scalar meson production case when the coupling constants of vector meson fields arefixed according to gNNp and fNNp in NN scattering and the SU(3) relation.

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What this paper is about

The cross sections ofΩ + Ξ→ (ΩΩ)Jπ=0+ + K(K*) and Ω + Ω→ (ΩΩ)Jπ 0+ + η(φ) are studied by using an effective Hamiltonian method.For the two pseudo-scalar meson production processes,the cross sections are still in the order of severalμbs,but for the two vector meson production processes,the cross sections are about 10 times larger than those in pseudo-scalar meson production case when the coupling constants of vector meson fields arefixed according to gNNp and fNNp in NN scattering and the SU(3) relation.

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Available abstract

The cross sections ofΩ + Ξ→ (ΩΩ)Jπ=0+ + K(K*) and Ω + Ω→ (ΩΩ)Jπ 0+ + η(φ) are studied by using an effective Hamiltonian method.For the two pseudo-scalar meson production processes,the cross sections are still in the order of severalμbs,but for the two vector meson production processes,the cross sections are about 10 times larger than those in pseudo-scalar meson production case when the coupling constants of vector meson fields arefixed according to gNNp and fNNp in NN scattering and the SU(3) relation.

Key concepts: Physics, Meson, Scalar (mathematics), Particle physics, Baryon, Vector meson, Scattering, Cross section (physics)

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