Contents: | Equilibrium Fractions |
Tab. 1 SH89d | |
Tab. 2 SH91c |
Y i+ + C → Y k+
Table 1 (Experiment)
K.Shima, N. Kuno, M. Yamanouchi // Phys. Rev. A v.40 p.3557 (1989)
E, MeV/amu | F 13 | F 14 | F 15 | F 16 | F 17 | F 18 | F 19 | F 20 | F 21 | F 22 | F 23 | F 24 | F 25 | F 26 | F 27 | F 28 | F 29 | F 30 | q av /Z | d | s |
0.581 | 0.0027 | 0.0141 | 0.0461 | 0.112 | 0.186 | 0.228 | 0.209 | 0.127 | 0.0542 | 0.0162 | 0.0035 | 0.0006 | — | — | — | — | — | — | 0.464 | 1.71 | 0.001 |
0.692 | 0.0007 | 0.0048 | 0.0211 | 0.0651 | 0.137 | 0.201 | 0.235 | 0.178 | 0.102 | 0.0406 | 0.0119 | 0.0026 | 0.0005 | — | — | — | — | — | 0.482 | 1.73 | 0.005 |
0.837 | — | 0.0011 | 0.0060 | 0.0266 | 0.0703 | 0.137 | 0.220 | 0.218 | 0.171 | 0.0951 | 0.0388 | 0.0126 | 0.0030 | 0.0007 | — | — | — | — | 0.505 | 1.77 | 0.040 |
0.994 | — | — | — | 0.0091 | 0.0278 | 0.0764 | 0.153 | 0.216 | 0.215 | 0.157 | 0.0890 | 0.0404 | 0.0124 | 0.0026 | — | — | — | — | 0.529 | 1.80 | 0.121 |
1.137 | — | — | — | 0.0029 | 0.0127 | 0.0418 | 0.102 | 0.183 | 0.216 | 0.181 | 0.136 | 0.0768 | 0.0332 | 0.0119 | 0.0028 | 0.0005 | — | — | 0.547 | 1.87 | 0.138 |
1.329 | — | — | — | — | 0.0032 | 0.0148 | 0.0490 | 0.100 | 0.167 | 0.187 | 0.191 | 0.140 | 0.0861 | 0.0422 | 0.0147 | 0.0044 | 0.0008 | — | 0.575 | 1.98 | 0.099 |
1.565 | — | — | — | — | — | 0.0028 | 0.0118 | 0.0365 | 0.0821 | 0.141 | 0.181 | 0.193 | 0.161 | 0.108 | 0.0562 | 0.0207 | 0.0061 | 0.0004 | 0.608 | 2.00 | -0.019 |
1.701 | — | — | — | — | — | — | 0.0049 | 0.0183 | 0.0493 | 0.101 | 0.154 | 0.188 | 0.188 | 0.149 | 0.0915 | 0.0409 | 0.0138 | 0.0015 | 0.626 | 1.98 | -0.050 |
Maximunm of F i (E) are marked by colour
Table 2 (Recommended data)
K.Shima, N. Kuno, M.Yamanouchi, H.Tawara // NIFS-DATA-10 (1991)
E, MeV/amu | q av | q av /Z | d |
0.02 | 5.280 | 0.135 | 2.070 |
0.04 | 6.820 | 0.175 | 1.980 |
0.1 | 9.720 | 0.249 | 1.810 |
0.2 | 12.80 | 0.328 | 1.620 |
0.4 | 16.32 | 0.418 | 1.660 |
1.0 | 20.65 | 0.539 | 1.870 |
2.0 | 25.91 | 0.664 | 1.940 |
4.0 | 30.79 | 0.789 | 1.450 |
6.0 | 32.71 | 0.839 | 1.450 |