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σ 4,5 DU04 SH11
σ 4,3 SH11
σ 4,6 DU04
σ 4,7 DU04
σ 4,8 DU04
σ 4,9 DU04
σ 4,10 DU04

U 4+ + N 2 → U 5+

Table 1 (Experiment)

R.D. DuBois, A.C.F. Santos, Th. Stohlker, et al. // Phys. Rev. A V.70, p.32712 (2004)

E , MeV/amu

σ 4,5 , 10 -16 cm 2 /atom
1.4 1.41

Error does not exceed 15 %

Table 2 (Theory, relativistic Born approximation)

V.P. Shevelko, I.L. Beigman, M.S. Litsarev, H. Tawara, I. Yu. Tolstikhina, G. Weber //Nucl. Instr. Methods Phys. Res. B V. 269, P.1455 (2011)

E , MeV/amu

σ 4,5 , 10 -16 cm 2 /atom
0.01 2.7
0.1 23.0
1.0 8.7
10.0 1.2
100.0 0.14
1000.0 0.032
1.e+4 0.023
1.e+5 0.022

U 4+ + N 2 → U 3+

Table 3 (Theory, OBK with normalization at low energy)

V.P. Shevelko, I.L. Beigman, M.S. Litsarev, H. Tawara, I. Yu. Tolstikhina, G. Weber //Nucl. Instr. Methods Phys. Res. B V. 269, P.1455 (2011)

E , MeV/amu

σ 4,3 , 10 -16 cm 2 /atom
0.01 123.0
0.02 90.0
0.03 67.0
0.05 44.0
0.07 29.0
0.1 16.0
0.2 6.0
0.3 2.3
0.5 0.58
0.7 0.23
1.0 0.060
2.0 0.010
3.0 2.5e-3
5.0 2.5e-4
7.0 6.6e-5
10.0 1.0e-5

U 4+ + N 2 → U 6+

Table 4 (Experiment)

R.D. DuBois, A.C.F. Santos, Th. Stohlker, et al. // Phys. Rev. A V.70, p.32712 (2004)

E , MeV/amu

σ 4,6 , 10 -16 cm 2 /atom
1.4 0.738

Error does not exceed 18 %

U 4+ + N 2 → U 7+

Table 5 (Experiment)

R.D. DuBois, A.C.F. Santos, Th. Stohlker, et al. // Phys. Rev. A V.70, p.32712 (2004)

E , MeV/amu

σ 4,7 , 10 -16 cm 2 /atom
1.4 0.517

Error does not exceed 5 %

U 4+ + N 2 → U 8+

Table 6 (Experiment)

R.D. DuBois, A.C.F. Santos, Th. Stohlker, et al. // Phys. Rev. A V.70, p.32712 (2004)

E , MeV/amu

σ 4,8 , 10 -16 cm 2 /atom
1.4 0.352

Error does not exceed 5 %

U 4+ + N 2 → U 9+

Table 7 (Experiment)

R.D. DuBois, A.C.F. Santos, Th. Stohlker, et al. // Phys. Rev. A V.70, p.32712 (2004)

E , MeV/amu

σ 4,9 , 10 -16 cm 2 /atom
1.4 0.170

Error does not exceed 5 %

U 4+ + N 2 → U 10+

Table 8 (Experiment)

R.D. DuBois, A.C.F. Santos, Th. Stohlker, et al. // Phys. Rev. A V.70, p.32712 (2004)

E , MeV/amu

σ 4,10 , 10 -16 cm 2 /atom
1.4 0.0334

Error does not exceed 21 %