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σ 1,0 | BA53 | JA53 | FI58 | FI60 | FI62 | MA62 | BR63 | CH63 | CH64 | MC63c | GI66 | BE67 | WI66 | FU76 | BE77c | BE77d | DE77 | SH78 | RE81 | HV82b | FU83 | WI84 | BE87b | GE87a | SC87 | SH89c | BA90 | SC90 | HA98 | TO99 | WI09 |
Figures
H + + H → H 0
Table 1 (Theory, OBK approximation)
D.R. Bates, A. Dalgarno // Proc. Phys. Soc. A v.66 p.972 (1953)
E, MeV/amu | σ 1,0 , π a02 | σ 1,0 , 10 -16 cm 2 |
0.0025 | 53.9 | 47.4 |
0.0079 | 15.3 | 13.5 |
0.025 | 3.42 | 3.01 |
0.079 | 0.229 | 0.201 |
0.250 | 3.2e-3 | 2.7e-3 |
0.790 | 1.2e-5 | 1.08e-5 |
2.5 | 2.3e-8 | 2.0e-8 |
7.9 | 3.1e-11 | 2.7e-11 |
Table 2 (Theory, Born approximation)
J.D.Jackson, H. Schiff // Phys. Rev. v.89 p.359 (1953)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.030 | 2.4 |
0.040 | 1.2 |
0.050 | 0.74 |
0.060 | 0.44 |
0.070 | 0.29 |
0.080 | 0.20 |
0.090 | 0.13 |
0.100 | 0.093 |
0.110 | 0.070 |
0.120 | 0.051 |
0.130 | 0.038 |
0.140 | 0.029 |
0.150 | 0.022 |
Table 3 (Experiment)
W.L. Fite, R.T.Brackmann, W.R.Snow // Phys. Rev., 112, 1161 (1958)
H.Tawara, T.Kato, Y.Nakai // At.Data Nucl.Data Tab. V.23 p.235 (1985)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.000024 | 29.0 |
0.000031 | 30.4 |
0.000040 | 28.1 |
0.000048 | 25.4 |
0.000060 | 22.9 |
0.000076 | 22.9 |
0.000090 | 21.5 |
0.000109 | 20.3 |
0.000116 | 20.7 |
0.000160 | 18.8 |
0.000203 | 17.3 |
0.000250 | 15.9 |
0.000303 | 15.0 |
0.000360 | 14.5 |
0.000400 | 14.3 |
0.000578 | 12.7 |
0.000706 | 12.2 |
0.000903 | 10.4 |
0.00132 | 8.0 |
0.00156 | 5.6 |
Table 4 (Experiment)
W.L. Fite, R.F.Stebbings, D.G.Hummer, R.T.Brackmann // Phys. Rev., 119, 663 (1960)
H.Tawara, T.Kato, Y.Nakai // At.Data Nucl.Data Tab. V.23 p.235 (1985)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.0004 | 26.0 ± 5.0 |
0.0010 | 20.0 ± 3.0 |
0.0018 | 17.0 ± 2.5 |
0.0036 | 14.0 ± 2.0 |
0.0070 | 10.5 ± 1.5 |
0.0100 | 9.0 ± 1.5 |
0.0200 | 6.4 ± 1.0 |
0.0300 | 4.1 ± 0.7 |
0.0400 | 3.1 ± 0.6 |
Table 5 (Experiment)
W.L. Fite, A.C.H. Smith, R.F.Stebbings // Proc. Roy. Soc., A 268, 527 (1962)
H.Tawara, T.Kato, Y.Nakai // At.Data Nucl.Data Tab. V.23 p.235 (1985)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.000019 | 43.0 ± 4.0 |
0.000022 | 36.0 ± 3.0 |
0.000023 | 40.0 |
0.000030 | 36.0 ± 3.0 |
0.000036 | 36.0 |
0.000038 | 32.0 ± 2.0 |
0.000046 | 33.0 |
0.000055 | 35.0 |
0.000060 | 32.0 ± 1.0 |
0.000076 | 27.0 |
0.00010 | 31.0 |
0.000107 | 31.0 ± 1.0 |
0.000143 | 26.0 |
0.000200 | 28.0 |
0.000230 | 23.0 ± 2.0 |
0.000300 | 25.0 ± 2.0 |
0.000470 | 22.0 ± 2.0 |
0.000610 | 21.0 |
0.000660 | 21.0 ± 2.0 |
0.000820 | 21.0 |
0.00100 | 19.0 |
0.00145 | 20.0 ± 4.0 |
0.00195 | 17.0 |
Table 6 (Theory, Born approximation)
R. A. Mapleton // Phys. Rev. v.126 p.1477 (1962)
E, MeV/amu | σ 1,0 , π a02 | σ 1,0 , 10 -16 cm 2 |
0.03162 | 0.0417 | 0.0368 |
0.05623 | 7.00e-3 | 6.16e-3 |
0.100 | 7.96e-4 | 7.00e-4 |
0.1778 | 6.39e-5 | 5.63e-5 |
0.3162 | 3.89e-6 | 3.42e-6 |
0.5623 | 1.92e-7 | 1.69e-7 |
1.0 | 8.14e-9 | 7.16e-9 |
Table 7 (Theory, Impulse approximation)
B. H. Bransden, I.M. Cheshire // Proc. Phys. Soc. v.81 p.820 (1963)
E, MeV/amu | σ 1,0 , π a02 | σ 1,0 , 10 -16 cm 2 |
0.025 | 3.8 | 3.34 |
0.050 | 1.4 | 1.23 |
0.100 | 0.26 | 0.229 |
0.150 | 0.072 | 0.0633 |
0.200 | 0.020 | 0.0176 |
0.400 | 1.8e-3 | 1.58e-3 |
0.600 | 2.4e-4 | 2.11e-4 |
0.800 | 5.5e-5 | 4.84e-5 |
1.0 | 2.0e-5 | 1.76e-5 |
Table 8 (Theory, Impulse approximation)
I.M. Cheshire // Proc. Phys. Soc. v.82 p.113 (1963)
E, MeV/amu | σ 1,0 (1s,1s), π a02 | σ 1,0 (1s,1s), 10 -16 cm 2 |
0.030 | 1.57 | 1.38 |
0.06324 | 0.225 | 0.198 |
0.11246 | 0.0329 | 0.0289 |
0.200 | 3.14e-3 | 2.76e-3 |
0.3556 | 2.25e-4 | 1.98e-4 |
0.6324 | 1.21e-5 | 1.06e-5 |
1.1236 | 5.97e-7 | 5.25e-7 |
Table 9 (Theory,CDW approximation)
I.M. Cheshire // Proc. Phys. Soc. v.84 p.89 (1964)
E, MeV/amu | σ 1,0 (1s,1s), π a02 | σ 1,0 (1s,1s), 10 -16 cm 2 |
0.0001 | 6.85e+5 | 6.03e+5 |
0.001 | 6700. | 5890. |
0.005 | 243. | 214. |
0.015 | 20.8 | 18.3 |
0.025 | 5.83 | 5.12 |
0.050 | 0.789 | 0.694 |
0.075 | 0.208 | 0.183 |
0.100 | 0.0733 | 0.0645 |
0.200 | 4.31e-3 | 3.79e-3 |
0.300 | 6.77e-4 | 5.96e-4 |
0.400 | 1.69e-4 | 1.49e-4 |
0.500 | 5.55e-5 | 4.88e-5 |
1.0 | 1.49e-6 | 1.31e-6 |
Table 10 (Theory,OBK approximation)
I.M. Cheshire // Proc. Phys. Soc. v.84 p.89 (1964)
E, MeV/amu | σ 1,0 (1s,1s), π a02 | σ 1,0 (1s,1s), 10 -16 cm 2 |
0.0001 | 1.27e+4 | 1.12e+4 |
0.001 | 1220. | 1070. |
0.005 | 201. | 176. |
0.015 | 4.24 | 3.73 |
0.025 | 1.68 | 1.48 |
0.050 | 3.37 | 2.96 |
0.075 | 1.04 | 0.915 |
0.100 | 0.400 | 0.352 |
0.200 | 0.0263 | 0.0231 |
0.300 | 4.17e-3 | 3.67e-3 |
0.400 | 1.02e-3 | 0.897e-3 |
0.500 | 3.29e-4 | 2.89e-4 |
1.0 | 7.95e-6 | 6.99e-6 |
Table 11 (Theory,Born approximation)
I.M. Cheshire // Proc. Phys. Soc. v.84 p.89 (1964)
E, MeV/amu | σ 1,0 (1s,1s), π a02 | σ 1,0 (1s,1s), 10 -16 cm 2 |
0.025 | 2.30 | 2.02 |
0.050 | 0.520 | 0.457 |
0.075 | 0.177 | 0.156 |
0.100 | 0.0734 | 0.0645 |
0.200 | 6.01e-3 | 5.29e-3 |
0.300 | 1.08e-3 | 0.950e-3 |
0.400 | 2.92e-4 | 2.57e-4 |
0.500 | 1.00e-4 | 0.880e-4 |
1.0 | 2.94e-6 | 2.59e-6 |
Table 12 (Experiment)
M.B. McElroy // Proc. Roy. Soc.A v.272 p.542 (1963)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.025 | 3.69 |
0.050 | 1.06 |
0.1 | 0.161 |
0.2 | 0.0133 |
0.4 | 6.48e-4 |
0.8 | 2.05e-5 |
Table 13 (Experiment)
H.B. Gilbody, G. Ryding // Proc. Roy. Soc. A v.291, p.438 (1966)
E, MeV/amu | σ 1,0 , π a02 | σ 1,0 , 10 -16 cm 2 |
0.038 | 2.5 ± 0.6 | 2.2 ± 0.5 |
0.043 | 1.6 ± 0.4 | 1.4 ± 0.3 |
0.048 | 0.68 ± 0.10 | 0.59 ± 0.09 |
0.058 | 0.48 ± 0.06 | 0.42 ± 0.05 |
0.068 | 0.32 ± 0.06 | 0.28 ± 0.05 |
0.078 | 0.24 ± 0.04 | 0.21 ± 0.03 |
0.088 | 0.18 ± 0.03 | 0.16 ± 0.03 |
0.098 | 0.12 ± 0.02 | 0.11 ± 0.02 |
0.108 | 0.086 ± 0.016 | 0.076 ± 0.014 |
0.118 | 0.076 ± 0.016 | 0.067 ± 0.014 |
0.128 | 0.049 ± 0.011 | 0.043 ± 0.010 |
Table 14 (Experiment)
V.A. Belyaev, B.G. Brezhnev, E.M. Erastov // Zh.Eksp.Teor.Fiz. 52, 1170 (1967)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
3.0e-6 | 55. ± 5. |
4.5e-6 | 52. ± 8. |
9.0e-6 | 46. ± 5. |
15.0e-6 | 45. ± 3. |
20.0e-6 | 47. ± 4. |
25.0e-6 | 44. ± 3. |
30.0e-6 | 41. ± 3. |
40.0e-6 | 40. ± 2. |
45.0e-6 | 39. ± 3. |
Table 15 (Experiment)
A.B.Wittkower, G.Ryding, H.B. Gilbody // Proc. Phys. Soc. v.89 p.541 (1966)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.040 | 2.0 |
0.060 | 0.68 |
0.067 | 0.51 ±0.06 |
0.070 | 0.40 |
0.080 | 0.27 ±0.08 |
0.090 | 0.16 |
0.100 | 0.12 |
0.110 | 0.070 ±0.027 |
0.125 | 0.051 |
0.150 | 0.023 |
0.175 | 0.013 |
0.200 | 0.0072 |
0.225 | 0.0043 |
0.250 | 0.0019 |
Table 16 (Theory, Brinkman-Kramers approximation)
K. Fujiwara // J.Phys.Soc.Jap. v.41 p.1350 (1976)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.04 | 5.234 |
0.06 | 1.789 |
0.08 | 0.7449 |
0.10 | 0.3519 |
0.12 | 0.1821 |
0.14 | 0.1010 |
Table 17 (Theory, continuum distorted-wave (CDW) approximation)
Dz. Belkic, R. Gayet // J.Phys. B v.10 p.1911 (1977)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.025 | 6.8 |
0.030 | 4.4 |
0.040 | 2.1 |
0.050 | 1.0 |
0.070 | 0.35 |
0.100 | 9.5e-2 |
0.150 | 1.9e-2 |
0.200 | 4.9e-3 |
0.250 | 1.8e-3 |
0.300 | 7.1e-4 |
0.400 | 1.9e-4 |
0.500 | 6.5e-5 |
0.700 | 1.1e-5 |
1.000 | 1.8e-6 |
1.500 | 1.7e-7 |
2.000 | 3.3e-8 |
2.500 | 1.0e-8 |
Table 18 (Theory, continuum intermediate-state (CIS) approximation)
Dz. Belkic // J.Phys. B v.10 p.3491 (1977)
E, MeV/amu | σ 1,0 , π ao2 | σ 1,0 , 10 -16 cm 2 |
0.050 | 1.34 | 1.18 |
0.100 | 1.26e-1 | 1.10e-1 |
0.250 | 2.73e-3 | 2.40e-3 |
0.500 | 9.51e-5 | 8.37e-5 |
0.750 | 1.16e-5 | 1.02e-5 |
1.000 | 2.51e-6 | 2.21e-6 |
2.500 | 1.59e-8 | 1.40e-8 |
5.000 | 3.13e-10 | 2.75e-10 |
7.500 | 3.09e-11 | 2.72e-11 |
10.000 | 5.96e-12 | 5.24e-12 |
Table 19 (Theory,Eikonal approximation )
D.P.Dewangan // J.Phys. B v.10 p.1083 (1977)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.020 | 1.6 |
0.060 | 0.258 |
0.100 | 6.47e-2 |
0.200 | 5.48e-3 |
0.400 | 2.60e-4 |
0.500 | 8.81e-5 |
0.900 | 4.32e-6 |
1.000 | 2.5e-6 |
1.500 | 2.7e-7 |
2.000 | 5.6e-8 |
2.500 | 1.6e-8 |
Table 20 (Theory,AO method )
R. Shakeshaft // Phys. Rev. A v.18 p.1930 (1978)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.015 | 6.63 |
0.025 | 3.76 |
0.040 | 1.59 |
0.050 | 0.918 |
0.060 | 0.553 |
0.075 | 0.278 |
0.145 | 0.0253 |
0.200 | 0.00607 |
Table 21 (Theory - single-centred expansion method )
J.F. Reading, A.L. Ford, R.L. Becker // J. Phys. B v.14 p.1995 (1981)
E , MeV/amu |
σ 1,0 , 10 -16 cm 2 |
0.015 | 6.3 |
0.030 | 2.8 |
0.060 | 0.5 |
0.100 | 0.094 |
Table 22 (Experiment)
P. Hvelplund, A. Andersen // Phys.Scr. v.26 p.375 (1982)
E , MeV/amu |
σ 1,0 , 10 -16 cm 2 |
0.25 | (1.65 ± 0.25) e-3 |
0.40 | (1.55 ± 0.28) e-4 |
0.50 | (5.45 ± 1.00) e-5 |
0.60 | (1.87 ± 0.36) e-5 |
Table 23 (Theory, AO method)
K. Fujiwara, N.Toshima // J.Phys.Soc.Jap. v.52 p.4118 (1983)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.10 | 0.120 |
0.30 | 1.88e-3 |
1.0 | 5.64e-6 |
2.0 | 1.30e-7 |
4.0 | 2.49e-9 |
5.625 | 3.42e-10 |
Table 24 (Theory, coupled-state method)
T.G. Winter, C.D. Lin // Phys. Rev. A v.29 p.567 (1984)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.00156 | 15.2 |
0.00300 | 12.9 |
0.00516 | 10.5 |
0.00800 | 9.02 |
0.01111 | 7.78 |
0.015 | 6.31 |
Table 25 (Theory - Boundary corrected first Born (CB1) approximation)
Dz. Belkic // Phys.Rev. A v.36 p.1601 (1987)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.020 | 4.49 |
0.025 | 3.11 |
0.030 | 2.23 |
0.040 | 1.23 |
0.050 | 0.730 |
0.060 | 0.455 |
0.070 | 0.295 |
0.075 | 0.241 |
0.080 | 0.198 |
0.090 | 0.137 |
0.100 | 0.0968 |
0.200 | 7.25e-3 |
0.300 | 1.26e-3 |
0.400 | 3.31e-4 |
0.500 | 1.12e-4 |
0.600 | 4.53e-5 |
0.700 | 2.07e-5 |
0.800 | 1.03e-5 |
0.900 | 5.58e-6 |
1.000 | 3.19e-6 |
1.500 | 3.55e-7 |
2.000 | 7.21e-8 |
3.500 | 3.06e-9 |
Table 26 (Experiment)
M.W. Gealy, B.V. Zyl // Phys.Rev. A v.36 p.3091 (1987)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.000063 | 0.334 ± 0.087 |
0.000088 | 0.345 ± 0.055 |
0.000125 | 0.423 ± 0.072 |
0.000177 | 0.537 ± 0.113 |
0.000250 | 0.790 ± 0.110 |
0.000354 | 1.19 ± 0.17 |
0.000500 | 1.92 ± 0.27 |
0.000707 | 3.05 ± 0.40 |
0.001000 | 4.43 ± 0.62 |
0.001414 | 5.86 ± 0.76 |
0.002000 | 6.95 ± 0.63 |
Table 27 (Experiment)
W.Schwab, G.B.Baptista, E.Justiniano, R.Schuch, H.Vogt, E.W. Weber // J.Phys. B v.20 p.2825 (1987)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
2.0 | (5.25 ± 2.25) e-8 |
3.5 | (2.14 ± 0.20) e-9 |
5.0 | (3.10 ± 0.60) e-10 |
7.5 | (4.10 ± 1.10) e-11 |
Table 28 (Theory - AO method)
R.Shingal, C.D.Lin // Phys.Rev. A v.40 p.1302 (1989)
E, MeV/amu | σ 1,0 , 10 -16 cm 2 |
0.001 | 17.18 |
0.010 | 8.54 |
0.025 | 3.93 |
0.050 | 0.73 |
0.100 | 0.12 |
0.125 | 0.058 |
0.150 | 0.032 |
0.175 | 0.018 |
0.200 | 0.011 |
0.250 | 0.0046 |
0.300 | 0.0022 |
0.400 | 0.0006 |
Table 29 (Recommended data)
C.F. Barnett // Atomic Data for Fusion. V.1, ORNL-6086 (1990).
E , MeV/amu |
σ 1,0 , 10 -16 cm 2 |
1.2e-7 | 49.6 |
2.e-7 | 47.0 |
4.e-7 | 44.5 |
7.e-7 | 42.4 |
1.e-6 | 41.0 |
2.e-6 | 38.3 |
4.e-6 | 35.8 |
7.e-6 | 33.3 |
1.e-5 | 31.7 |
2.e-5 | 29.3 |
4.e-5 | 27.0 |
7.e-5 | 25.4 |
1.e-4 | 24.4 |
2.e-4 | 22.2 |
4.e-4 | 20.3 |
7.e-4 | 18.8 |
0.001 | 17.1 |
0.002 | 14.4 |
0.004 | 12.0 |
0.007 | 9.42 |
0.01 | 7.75 |
0.02 | 4.45 |
0.04 | 1.67 |
0.07 | 0.377 |
0.1 | 0.101 |
0.2 | 6.09e-3 |
0.4 | 1.76e-4 |
0.63 | 1.35e-5 |
Table 30 (Theory - Claccical trajectory Monte Carlo calculations )
A. Schmidt, M. Horbatsch, R.M. Dreizler // J. Phys.B v.23 p.2327S (1990)
E , MeV/amu |
σ 1,0 , 10 -16 cm 2 |
0.01 | 4.8 |
0.02 | 3.6 |
0.03 | 2.8 |
0.05 | 1.0 |
0.07 | 0.33 |
0.1 | 0.12 |
0.2 | 0.010 |
0.3 | 0.0012 |
0.5 | 7.6e-5 |
Table 31 (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 1,0 , 10 -16 cm 2 |
0.0000625 | 0.05 | 29.5 |
0.00025 | 0.10 | 22.8 |
0.00100 | 0.20 | 17.3 |
0.00225 | 0.30 | 14.2 |
0.00400 | 0.40 | 11.9 |
0.00625 | 0.50 | 10.3 |
0.00900 | 0.60 | 9.17 |
0.01225 | 0.70 | 7.99 |
0.01600 | 0.80 | 6.77 |
0.02025 | 0.90 | 5.60 |
0.02500 | 1.00 | 4.55 |
Table 32 (Theory - close-coupling scheme based on an eikonal-distorted-wave expansion. )
N. Toshima, T. Nakagawa // Phys.Rev. A v.60 p.2182 (1999)
E , MeV/amu |
σ 1,0 , 10 -16 cm 2 |
0.01 | 8.0 |
0.05 | 0.56 |
0.10 | 0.056 |
0.15 | 0.014 |
0.20 | 4.7e-3 |
0.25 | 1.7e-3 |
0.30 | 7.7e-4 |
0.35 | 3.7e-4 |
0.40 | 2.0e-4 |
Table 33 (Theory - Atomic orbital method with Sturmian-pseudostate bases )
T.G. Winter // Phys. Rev. A v.80 p.032701 (2009)
E , MeV/amu |
σ 1,0 , 10 -16 cm 2 |
0.0010 | 17.31 |
0.001563 | 15.60 |
0.0030 | 13.11 |
0.0040 | 11.81 |
0.00516 | 10.75 |
0.008 | 9.358 |
0.015 | 6.732 |
0.025 | 3.942 |
0.050 | 1.003 |
0.075 | 0.303 |
0.100 | 0.111 |