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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Extra info for Clustering Aspects of Quantum Many-Body Systems
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.