Three-body-model calculations for C-22

Kucuk Y., Tostevin J. A.

Rutherford Centennial Conference on Nuclear Physics, Manchester, Birleşik Krallık, 8 - 12 Ağustos 2011, cilt.381 identifier identifier

  • Yayın Türü: Bildiri / Tam Metin Bildiri
  • Cilt numarası: 381
  • Doi Numarası: 10.1088/1742-6596/381/1/012109
  • Basıldığı Şehir: Manchester
  • Basıldığı Ülke: Birleşik Krallık
  • Akdeniz Üniversitesi Adresli: Hayır

Özet

There are now several well-studied instances where very neutron-rich light nuclei at or near the neutron drip-line, such as 6He, 11Li and 14Be, have been found to have a Borromean three-body structure. Such systems are modelled effectively as a well-bound core nucleus plus two weakly-bound valence neutrons, where none of the two-body subsystems forms a bound state. It is now known that the heaviest particle-bound carbon isotope, 22C, shares these properties. We discuss a development of four-body reaction model calculations, using the fast adiabatic approximation, that is particularly well-suited for a quantitative analysis of reactions of such neutron-rich nuclei with a target nucleus at beam energies of order 100-300 MeV per nucleon; energies available at new and future radioactive ion beam (RIB) facilities. The 22C projectile wave function is calculated using the 20C core plus two-valence neutron three-body description.

 
There are now several well-studied instances where very neutron-rich light nuclei at or near the neutron drip-line, such as He-6, Li-11 and Be-14, have been found to have a Borromean three-body structure. Such systems are modelled effectively as a well-bound core nucleus plus two weakly-bound valence neutrons, where none of the two-body subsystems forms a bound state. It is now known that the heaviest particle-bound carbon isotope, C-22, shares these properties. We discuss a development of four-body reaction model calculations, using the fast adiabatic approximation, that is particularly well-suited for a quantitative analysis of reactions of such neutron-rich nuclei with a target nucleus at beam energies of order 100-300 MeV per nucleon; energies available at new and future radioactive ion beam (RIB) facilities. The C-22 projectile wave function is calculated using the C-20 core plus two-valence neutron three-body description.