19 01, 2024

Researchers Apply No-core Gamow shell Model to Investigate First Excited State of α Particle

The α particle, also known as helium-4, consists of two protons and two neutrons. Although it is one of the most extensively studied atomic nuclei, the precise nature of its excited states remains unclear. A recent precise experimental study about the first excited state of helium-4, which is labeled 0+(2) by scientists, has raised a new debate due to a large discrepancy between experiment data and theoretical predictions.

To better understand the nature of this state, Prof. Nicolas Michel from the Institute of Modern Physics (IMP) of the Chinese Academy of Sciences (CAS) and his collaborators M. Ploszajczak (GANIL, France) and W. Nazarewicz (MSU, USA ) have employed the no-core Gamow shell model to study the structure of the resonance 0+(2) state of helium-4. The research was published in Physical Review Letters and highlighted as a “Featured in Physics” article. 

The 0+(2) state of helium-4 is only unbound by about 410 keV. It is a one-proton emitter, but has a very short life-time. The 0+(2) resonance has traditionally been viewed either as a breathing mode or as a particle-hole excitation of its helium-4 ground state. 

Michel and his collaborators have provided new descriptions for the 0+(2) state of helium-4. They predicted a rather complex structure for the 0+(2) resonance exhibiting a strong continuum coupling between the various decay channels. It was found that the continuum coupling strongly impacts the nature of this proton-emitting state. And they obtained the best agreement with experimental data for the monopole form factor at the experimental energy. 

Thus, the researchers suggest that the 0+(2) state should not be seen as a breathing oscillation or a particle-hole excitation, but on the contrary as a threshold-aligned broad resonance.

 

Figure. Advanced theoretical calculations predict a rather complex character of the excited 0+ state of the α particle at 20.21 MeV that involves a coupling between three binary cluster configurations. (Image by W. Nazarewicz)

DOI: https://doi.org/10.1103/PhysRevLett.131.242502 


Contact:

LIU Fang

Institute of Modern Physics

Email: fangliu@impcas.ac.cn

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LIU Fang

Institute of Modern Physics

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