Compositeness of baryonic resonances: Application to the Δ(1232), N(1535), and N(1650) resonances

被引:27
作者
Sekihara, Takayasu [1 ]
Arai, Takashi [2 ]
Yamagata-Sekihara, Junko [3 ]
Yasui, Shigehiro [4 ]
机构
[1] Osaka Univ, RCNP, Ibaraki, Osaka 5670047, Japan
[2] High Energy Accelerator Res Org KEK, IPNS, Theory Ctr, 1-1 Oho, Tsukuba, Ibaraki 3050801, Japan
[3] Oshima Coll, Natl Inst Technol, Yamaguchi 7422193, Japan
[4] Tokyo Inst Technol, Dept Phys, Tokyo 1528551, Japan
基金
日本学术振兴会;
关键词
CHIRAL DYNAMICS; NUCLEON INTERACTIONS; ELEMENTARY PARTICLE; REACTION AMPLITUDES; WAVE-FUNCTIONS; PI-N; STATES; SCATTERING; REPRESENTATION; CONSTRAINTS;
D O I
10.1103/PhysRevC.93.035204
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
We present a formulation of the compositeness for baryonic resonances to discuss the meson-baryon molecular structure inside the resonances. For this purpose, we derive a relation between the residue of the scattering amplitude at the resonance pole position and the two-body wave function of the resonance in a sophisticated way, and we define the compositeness as the norm of the two-body wave functions. As applications, we investigate the compositeness of the Delta(1232), N(1535), and N(1650) resonances from precise pi N scattering amplitudes in a unitarized chiral framework with the interaction up to the next-to-leading order in chiral perturbation theory. The pi N compositeness for the Delta(1232) resonance is evaluated in the pi N single-channel scattering, and we find that the pi N component inside Delta(1232) in the present framework is non-negligible, which supports the previous work. On the other hand, the compositeness for the N(1535) and N(1650) resonances is evaluated in a coupled-channel approach, resulting that the pi N, eta N, K Lambda, and K Sigma components are negligible for these resonances.
引用
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页数:22
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