{"qid": "D3111", "reaction": "e- + H2 X(1\u03a3+g);v=2 \u2192 H2 e(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": 13.6782, "fit": {"coeffs": {"A1": 2.6799e-05, "A2": 0.093067, "A3": -0.68814, "A4": 2.7385, "A5": -2.1953}, "func": "singlet_triplet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:32.224797+00:00"}
------------------------------------------------------------------------
1.368e+01 0.0
1.400e+01 1.561e-21
1.450e+01 2.254e-20
1.500e+01 5.867e-20
1.550e+01 1.704e-19
1.600e+01 4.165e-19
1.650e+01 6.529e-19
1.700e+01 8.026e-19
1.750e+01 8.882e-19
1.800e+01 9.356e-19
1.850e+01 9.341e-19
1.900e+01 9.247e-19
1.950e+01 9.08e-19
2.000e+01 8.825e-19
2.100e+01 8.219e-19
2.200e+01 7.704e-19
2.300e+01 7.164e-19
2.400e+01 6.641e-19
2.500e+01 6.144e-19
2.600e+01 5.68e-19
2.700e+01 5.252e-19
2.800e+01 4.859e-19
2.900e+01 4.499e-19
3.000e+01 4.171e-19
3.500e+01 2.91e-19
4.000e+01 2.098e-19
4.500e+01 1.559e-19
5.000e+01 1.188e-19
6.000e+01 7.363e-20
7.000e+01 4.877e-20
8.000e+01 3.399e-20
9.000e+01 2.465e-20
1.000e+02 1.845e-20
1.250e+02 9.947e-21
1.500e+02 5.978e-21