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Titlebook: Gamow Shell Model; The Unified Theory o Nicolas Michel,Marek P?oszajczak Book 2021 Springer International Publishing AG 2021 Gamow states i

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21#
發(fā)表于 2025-3-25 03:51:13 | 只看該作者
22#
發(fā)表于 2025-3-25 10:30:57 | 只看該作者
23#
發(fā)表于 2025-3-25 14:17:09 | 只看該作者
Physical Applications of the Gamow Shell Model, features of exotic nuclei that give prospects for entirely new phenomena likely to be different from anything we have observed to date. These phenomena can be described using the Gamow shell model. Certain specific features of interactions in weakly bound systems have been recently identified. In g
24#
發(fā)表于 2025-3-25 18:57:31 | 只看該作者
25#
發(fā)表于 2025-3-25 23:52:57 | 只看該作者
26#
發(fā)表于 2025-3-26 04:06:18 | 只看該作者
The Unification of Structure and Reaction Frameworks,from the same Hamiltonian. In standard reaction frameworks, the structure aspects of many-body nuclear states have been only indirectly included. For example, it is customary to use coupled-channel equations and one-body optical potentials to calculate reaction cross sections, whereby the parameters
27#
發(fā)表于 2025-3-26 06:51:41 | 只看該作者
The Discrete Spectrum and the Continuum,actions induced by the remaining .???1 nucleons. As a zeroth-order approximation, one can also deem these potentials as spherical, as the bulk properties of nuclei can be accounted for with spherical potentials.
28#
發(fā)表于 2025-3-26 10:40:48 | 只看該作者
Physical Applications of the Gamow Shell Model,na can be described using the Gamow shell model. Certain specific features of interactions in weakly bound systems have been recently identified. In general terms, these interactions depend explicitly on the location of various emission thresholds and on the structure of .-matrix poles which dominate the corresponding decays.
29#
發(fā)表于 2025-3-26 13:14:02 | 只看該作者
30#
發(fā)表于 2025-3-26 17:42:50 | 只看該作者
The Unification of Structure and Reaction Frameworks,example, it is customary to use coupled-channel equations and one-body optical potentials to calculate reaction cross sections, whereby the parameters entering one-body optical potentials are directly fitted from experimental data.
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