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| Figures | |||||||||
| σ 3,2 | SH78b | BE79 | RU79a | SE81 | FR82a | YA82 | BE87b | GR95 | HA98 |
Figures
Li 2+ + H → Li +
Table 1 (Experiment)
M.B.Shah, T.V. Goffe, H.B.Gilbody // J.Phys. B v.11 p.L233 (1978)
| E, MeV/amu | E, MeV | σ 3,2 , 10 -16 cm 2 |
| 0.014 | 0.100 | 15.6 ± 3.0 |
| 0.017 | 0.120 | 16.0 ± 3.0 |
| 0.023 | 0.160 | 14.1 ± 2.0 |
| 0.034 | 0.240 | 11.0 ± 2.0 |
| 0.046 | 0.320 | 7.1 ± 0.7 |
| 0.054 | 0.380 | 6.4 ± 1.0 |
| 0.060 | 0.420 | 4.7 ± 0.4 |
| 0.071 | 0.500 | 3.2 ± 0.6 |
| 0.079 | 0.550 | 2.3 ± 0.4 |
| 0.089 | 0.620 | 1.6 ± 0.3 |
| 0.096 | 0.675 | 1.5 ± 0.3 |
| 0.107 | 0.750 | 0.83 ± 0.15 |
| 0.129 | 0.900 | 0.53 ± 0.05 |
| 0.143 | 1.000 | 0.39 ± 0.07 |
| 0.171 | 1.200 | 0.13 ± 0.02 |
| 0.214 | 1.500 | 0.088 ± 0.012 |
Table 2 (Theory -Continuum distorted-wave approximation)
Dz.S.Belkic, R.Gayet, A.Salin // Phys.Rep. v.56 p.279 (1979)
| E, MeV/amu | E, MeV | σ 3,2 , 10 -16 cm 2 |
| 0.029 | 0.200 | 23.0 |
| 0.043 | 0.300 | 9.1 |
| 0.071 | 0.500 | 2.6 |
| 0.100 | 0.700 | 1.0 |
| 0.143 | 1.000 | 0.29 |
| 0.214 | 1.500 | 0.071 |
Table 3 (Theory - Distorted-wave Born approximation)
H.Ryufuku, T.Watanabe // Phys. Rev. A v.19 p.1538 (1979)
| E, MeV/amu | σ 3,2 , 10 -16 cm 2 |
| 0.000025 | 6.09 |
| 0.00005 | 7.19 |
| 0.0001 | 7.03 |
| 0.0002 | 8.05 |
| 0.0005 | 7.91 |
| 0.001 | 8.42 |
| 0.002 | 7.96 |
| 0.005 | 13.3 |
| 0.010 | 17.8 |
| 0.025 | 14.1 |
| 0.050 | 7.76 |
| 0.075 | 4.09 |
| 0.100 | 2.19 |
| 0.200 | 0.273 |
Table 4 (Experiment)
W.Seim, A. Muller, I.Wirkner-Bott, E.Salzborn // J. Phys. B, 14, 3475 (1981)
| E, MeV/amu | E, MeV | σ 3,2 , 10 -16 cm 2 |
| 0.00129 | 0.009 | 4.40 ± 1.05 |
| 0.00150 | 0.0105 | 4.50 ± 0.86 |
| 0.00171 | 0.012 | 4.73 ± 0.81 |
| 0.00193 | 0.0135 | 6.15 ± 1.06 |
| 0.00223 | 0.0156 | 6.40 ± 0.92 |
| 0.00257 | 0.018 | 7.60 ± 0.88 |
| 0.00300 | 0.021 | 8.30 ± 0.75 |
| 0.00343 | 0.024 | 9.00 ± 0.70 |
| 0.00386 | 0.027 | 9.60 ± 0.75 |
| 0.00429 | 0.030 | 10.7 ± 0.9 |
| 0.00471 | 0.033 | 12.4 ± 0.7 |
| 0.00540 | 0.0378 | 12.3 ± 0.8 |
| 0.00600 | 0.042 | 13.1 ± 1.4 |
Table 5 (Theory - AO method)
W.Fritsch, C.D. Lin // J.Phys. B v.15 p.L281 (1982)
W.Fritsch, C.D.Lin // Phys. Scr. v.T3 p.241 (1983)
| E, MeV/amu | E, MeV | σ 3,2 , 10 -16 cm 2 |
| 0.000429 | 0.003 | 1.69 |
| 0.000714 | 0.005 | 2.14 |
| 0.00100 | 0.007 | 2.64 |
| 0.00143 | 0.010 | 3.50 |
| 0.00214 | 0.015 | 5.15 |
| 0.00286 | 0.020 | 6.50 |
| 0.00500 | 0.035 | 10.7 |
| 0.00714 | 0.050 | 14.2 |
| 0.0100 | 0.070 | 16.3 |
| 0.0143 | 0.100 | 16.6 |
Table 6 (Theory - MO method)
T.O. Yamaguchi, Y.Itikawa // J.Phys.Soc.Jap. v.51 p.2982 (1982)
| E, MeV/amu | σ 3,2 , 10 -16 cm 2 |
| 0.0001 | 0.582 |
| 0.001 | 1.56 |
| 0.005 | 9.07 |
| 0.010 | 14.6 |
| 0.020 | 16.4 |
Table 7 (Theory - Boundary corrected first Born (CB1) approximation)
Dz. Belkic // Phys.Rev. A v.36 p.1601 (1987)
| E, MeV/amu | E, MeV | σ 3,2 , 10 -16 cm 2 |
| 0.00286 | 0.020 | 76.4 |
| 0.00429 | 0.030 | 57.9 |
| 0.00571 | 0.040 | 48.2 |
| 0.00857 | 0.060 | 39.0 |
| 0.0114 | 0.080 | 34.7 |
| 0.0129 | 0.090 | 33.2 |
| 0.0143 | 0.100 | 31.8 |
| 0.0286 | 0.200 | 19.6 |
| 0.0429 | 0.300 | 11.0 |
| 0.0571 | 0.400 | 6.22 |
| 0.0714 | 0.500 | 3.65 |
| 0.0857 | 0.600 | 2.23 |
| 0.100 | 0.700 | 1.42 |
| 0.114 | 0.800 | 0.936 |
| 0.129 | 0.900 | 0.637 |
| 0.143 | 1.000 | 0.445 |
| 0.179 | 1.250 | 0.201 |
| 0.214 | 1.500 | 0.101 |
| 0.286 | 2.000 | 0.0330 |
| 0.357 | 2.500 | 0.0135 |
Table 8 (Theory - Eikonal impulse approximation)
M.S. Gravielle, J.E. Miraglia // Phys.Rev. A v.51 p.2131 (1995)
| E, MeV/amu | E/i, MeV/amu | σ 3,2 , 10 -16 cm 2 |
| 0.260 | 0.020 | 4.3 |
| 0.150 | 0.050 | 0.29 |
| 0.210 | 0.070 | 0.10 |
| 0.300 | 0.100 | 0.022 |
| 0.450 | 0.150 | 3.9e-3 |
| 0.600 | 0.200 | 1.2e-3 |
Table 9 (Theory - Molecular close-coupling method)
C.Harel, H.Jouin, B.Pons // At.Data Nucl.Data Tab. v.68 p.279 (1998)
| E , MeV/amu |
V, a.u. |
σ 3,2 , 10 -16 cm 2 |
| 0.0000625 | 0.05 | 0.825 |
| 0.00025 | 0.1 | 1.30 |
| 0.00100 | 0.20 | 2.60 |
| 0.00225 | 0.30 | 5.63 |
| 0.00400 | 0.40 | 9.30 |
| 0.00625 | 0.50 | 14.2 |
| 0.00900 | 0.60 | 17.40 |
| 0.01225 | 0.70 | 19.10 |
| 0.01600 | 0.80 | 19.70 |
| 0.02025 | 0.90 | 19.2 |
| 0.02500 | 1.00 | 18.1 |