{"qid": "D3028", "reaction": "e- + H2 X(1\u03a3+g);v=9 \u2192 H2 b(3\u03a3+u) + e-", "process_types": {"EDE": "Dissociative Excitation"}, "data_type": "cross section", "refs": {"B10": {"doi": "10.1016/j.adt.2020.101361"}}, "comment": "MCCC calculations of vibrationally-resolved electron-impact dissociative excitation of H2, adiabatic nuclei calculations performed with the spheroidal MCCC(210) model", "method": "MCCC", "columns": [{"name": "E", "units": "eV"}, {"name": "sigma", "units": "cm2"}], "unc_perc": 10.0, "threshold": 0.864974, "fit": {"coeffs": {"A1": 6.646e+16, "A2": 2.2931, "A3": 37.725, "A4": 0.17}, "func": "EDE_b3Su"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:09.332674+00:00"}
------------------------------------------------------------------------
8.650e-01 0.0
1.000e+00 5.797e-19
1.500e+00 5.786e-17
2.000e+00 1.282e-16
2.500e+00 1.459e-16
3.000e+00 1.502e-16
3.500e+00 1.541e-16
4.000e+00 1.552e-16
4.500e+00 1.525e-16
5.000e+00 1.48e-16
5.500e+00 1.444e-16
6.000e+00 1.408e-16
6.500e+00 1.369e-16
7.000e+00 1.325e-16
7.500e+00 1.271e-16
8.000e+00 1.214e-16
8.500e+00 1.158e-16
9.000e+00 1.101e-16
9.500e+00 1.04e-16
1.000e+01 9.772e-17
1.050e+01 9.093e-17
1.100e+01 8.439e-17
1.150e+01 7.891e-17
1.200e+01 7.405e-17
1.250e+01 6.961e-17
1.300e+01 6.566e-17
1.350e+01 6.231e-17
1.400e+01 5.923e-17
1.450e+01 5.611e-17
1.500e+01 5.313e-17
1.550e+01 5.028e-17
1.600e+01 4.749e-17
1.650e+01 4.486e-17
1.700e+01 4.247e-17
1.750e+01 4.029e-17
1.800e+01 3.823e-17
1.850e+01 3.632e-17
1.900e+01 3.455e-17
1.950e+01 3.295e-17
2.000e+01 3.151e-17
2.100e+01 2.893e-17
2.200e+01 2.66e-17
2.300e+01 2.449e-17
2.400e+01 2.258e-17
2.500e+01 2.084e-17
2.600e+01 1.926e-17
2.700e+01 1.78e-17
2.800e+01 1.645e-17
2.900e+01 1.517e-17
3.000e+01 1.396e-17
3.500e+01 9.806e-18
4.000e+01 7.618e-18
4.500e+01 6.017e-18
5.000e+01 5.09e-18
6.000e+01 3.909e-18
7.000e+01 2.77e-18
8.000e+01 2.006e-18
9.000e+01 1.447e-18
1.000e+02 1.049e-18
1.250e+02 5.241e-19
1.500e+02 2.805e-19