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One- and two- neutron halo at the dripline. From $^{11}$Be to $^{11}$Li and back: $^{10}$Li and parity inversion
The nuclei $^{11}$Be and $^{11}$Li provide paradigmatic examples of one-and two- neutron halo systems. Because the reaction $^{1}$H($^{11}$Li,$^{9}$Li)$^{3}$H is dominated by successive transfer, one can use the quantitative picture emerging from a nu- clear field theory description of the structure...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2019
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/2669048 |
Sumario: | The nuclei $^{11}$Be and $^{11}$Li provide paradigmatic examples of one-and two- neutron halo systems. Because the reaction $^{1}$H($^{11}$Li,$^{9}$Li)$^{3}$H is dominated by successive transfer, one can use the quantitative picture emerging from a nu- clear field theory description of the structure and reaction mechanism of the above Cooper pair transfer process and of the $^{2}$H($^{10}$Be,$^{11}$Be)$^{1}$H and $^{1}$H($^{11}$Be,$^{10}$Be)$^{2}$H reactions, to shed light on the structure of $^{10}$Li. This analysis provides important support for a parity inverted scenario with a 1/2$^{+}$ virtual state at about 0.2 MeV. |
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