Fig. 1. Density distributions of 44Mg[17](a) The proton (x<0) and the neutron (x>0) densities, (b) The density of the neutron core, (c) The density of the neutron halo
Fig. 3. Neutron halo, neutron core, and neutron density distributions of 0+, 2+, and 4+ states of 44Mg by using the DRHBc theory with angular momentum projection
双(单)中子分离能S2n (Sn) / MeVTwo- (one-) neutron separation energy
均方根半径Rm / fmRoot-mean-square matter radius
s-波占比Amplitude of s-wave
DRHBc
实验值Experimental value
DRHBc
实验值Experimental value
DRHBc
17B
0.52
1.78
1.38(21)
3.03
3.00(6)[64]
14%
19B
0.36
0.22
0.089(56)
3.27
3.11(13)[64]
36%
15C
0.26
1.22
1.218 1(8)
2.64
2.54(4)[65]
36%
19C*
0.37
0.04
0.563 3(915)
3.05
3.16(7)[65]
66%
22C
-0.26
0.40
0.035(20)
3.25
3.44(8)[66]
25%
Table 1. Quadrupole deformation parameter, two- or one- neutron separation energy, root-mean-square matter radius, and the amplitude of s-wave components of the halo nuclei in born and carbon isotopes from the DRHBc calculations with the density functional PK1[62]. Available experimental values are included for comparison. The experimental data of neutron-separation energies are taken from AME2020[63]