Comment on "New modes of halo excitations in the 6He nucleus"
| dc.creator | Fedorov, D. V. | |
| dc.creator | Cobis, A. | |
| dc.creator | Jensen, A. S. | |
| dc.date | 1998-01-19 | |
| dc.date.accessioned | 2026-07-07T11:11:32Z | |
| dc.date.available | 2026-07-07T11:11:32Z | |
| dc.description | We try to explain the differences in the 6He dipole strength function in refs. [1] and [2]. We perform the full basis calculation of the strength function with the same renormalized interaction as in [1] and show that the size of the basis, needed for converged calculations of the 6He continuum spectrum, is much larger than that for the discrete spectrum. The renormalized interaction of [1] therefore cannot be used for the continuum spectrum calculations with the same basis as for the ground state. | |
| dc.description | 2 pages, 3 figures | |
| dc.identifier | https://arxiv.org/abs/nucl-th/9801033 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/9801033 | |
| dc.identifier | Phys.Rev.C59:554-555,1999 | |
| dc.identifier | doi:10.1103/PhysRevC.59.554 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/191127 | |
| dc.subject | Nuclear Theory | |
| dc.title | Comment on "New modes of halo excitations in the 6He nucleus" | |
| dc.type | text |