Nuclear Many-Body Theory

Welcome

A nucleus is a quantum many-body system consisting of two types of fermions, neutrons and protons, called nucleons, which are self-bound by a strong nuclear force. The number of constituent nucleons ranges from a few to a few hundred. Although the number is not very large, the nuclei exhibit various collective behaviors. Surprisingly, it is well established that the concept of single-particle motion in a mean field holds in nuclear structures despite the strong interaction between nucleons. The potential is collectively generated by all nucleons constituting the nucleus. The single-particle picture of the shell model, like electrons in an atom, emerges as a result of the collective effects of all nucleons generating the self-consistent mean field. In addition, some nuclei show a pattern of vibrational or rotational excitations as a whole, and some exhibit characteristic features of superfluids. We develop computational approaches based on quantum many-body theories to comprehensively delineate the intricate collective behaviors exhibited by nuclei. We welcome you to join us to explore the world of quantum nuclear systems.

What's new

"Nuclear mass table in density functional approach inspired by neutron-star observations", arXiv:2304.01546.

"Analysis of a Skyrme energy density functional with deep learning", PRC108, 034311 (2023).

"Electron wave functions in beta-decay formulas revisited (II): Completion including recoil-order and induced currents", PTEP2023.073D02.

"β-decay half-lives as an indicator of shape-phase transition in neutron-rich Zr isotopes with particle-vibration coupling effect", arXiv:2307.00817.

"Analysis of a Skyrme energy density functional with deep learning", arXiv:2306.11314.

"Triaxial-shape dynamics in the low-lying excited 0+ state: Role of the collective mass", arXiv:2304.11918.

"Electron wave functions in beta-decay formulas revisited (II): Completion including recoil-order and induced currents", arXiv:2303.08332.