7.5 Mirror Nuclei and Isospin Symmetry Breaking
355
Fig. 7.16 Distributions of real (upper) and imaginary (lower) parts of S c for 6 He (solid line) and
6 Be (dotted line) as a function of the Re[k] value of scattering states 3/2 − of the 5 He and 5 Li
nuclei. Calculations have been done for three different values of the threshold energy E T of the
A = 5 particle nuclei, which is −1.5 MeV (upper panel), 0 (middle panel), and 0.5 MeV (lower
panel). Arrows indicate the contributions of resonant state, multiplied by a scaling factor equal to
0.05 unless precised differently on the figure (from Ref. [112])
355
Fig. 7.16 Distributions of real (upper) and imaginary (lower) parts of S c for 6 He (solid line) and
6 Be (dotted line) as a function of the Re[k] value of scattering states 3/2 − of the 5 He and 5 Li
nuclei. Calculations have been done for three different values of the threshold energy E T of the
A = 5 particle nuclei, which is −1.5 MeV (upper panel), 0 (middle panel), and 0.5 MeV (lower
panel). Arrows indicate the contributions of resonant state, multiplied by a scaling factor equal to
0.05 unless precised differently on the figure (from Ref. [112])