Clustering Aspects of Quantum Many-Body Systems by A. Ohnishi, N. Itagaki, Y. Kanada-En'Yo, K. Kato

By A. Ohnishi, N. Itagaki, Y. Kanada-En'Yo, K. Kato

This court cases quantity comprises all of the invited talks and oral displays on the foreign Symposium on Clustering features of Quantum Many-Body structures, 12-14 November 2001, held in Kyoto, Japan. It discusses numerous positive factors of clustering features - localization of debris in static and dynamical contexts - of nuclear and atomic platforms. It additionally provides many theoretical advancements in quantum few-body and many-body difficulties. The paintings can be important to graduate scholars and researchers within the box of quantum many-body difficulties, particularly to those that are looking to comprehend the approach houses past the mean-field description.

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It is necessary to confirm the contribution of the nuclear interaction from the target nucleus. References 1. 2. 3. 4. 5. 6. T. T. T. F. T. C. ,Phys. Lett. B 331, 296 (1994) Myo, A. Ohnishi, and K. Kato, Prog. Theor. Phys. 99(1998),801. Berggren, Nucl. Phys. A109(l 968)265. Ajzenberg-selove, Nucl. Phys. A506( 1989)1. ,Phys. Lett. B 394, 11 (1997) A. Bertulani and G. Baur, Phys. l63(1988)299. CLUSTER STRUCTURE IN HYPERNUCLEI This page is intentionally left blank S T R U C T U R E OF LIGHT H Y P E R N U C L E I S T U D I E D B Y GAMMA-RAY SPECTROSCOPY H.

1(a). Here, the yield of the coincidence event was normalized to the singles yield taking into account the solid angles of SSD's. 7 MeV. The number of low energy tritons, which is possible to be lost due to the detector threshold, was estimated to be small. 3 Discussion In order to evaluate a branching ratio of the binary triton decay from the EX=1S MeV peak, we analyzed the singles spectrum with a least x 2 method. In this analysis, the previously reported resonances and the presently observed ^ = 1 8 MeV peak were taken into account.

1 On the other hand, the other terms, namely, the spin-spin t e r m Va, the A-spindependent spin-orbit term V\, the nucleon-spin-dependent spin-orbit t e r m VJV, and the tensor t e r m Vr, have not been well know. Since the Ap scattering d a t a are not available at all for these spin-dependent interactions, various baryon-baryon interaction models give different predictions. In shell-model description, low-lying level energies of p-shell hypernuclei with a A in the Os orbit can be described with five radial integrals for sAp^ wavefunction on the five terms in Eq.

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