{"qid": "D3087", "reaction": "e- + H2 X(1\u03a3+g);v=8 \u2192 H2 D(1\u03a0u) + 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": 13.2439, "fit": {"coeffs": {"A1": 0.43716, "A2": 0.34935, "A3": -2.3204, "A4": 5.4397, "A5": -5.5706, "A6": 2.1106}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:25.532761+00:00"}
------------------------------------------------------------------------
1.324e+01 0.0
1.350e+01 2.229e-22
1.400e+01 4.97e-21
1.450e+01 1.927e-20
1.500e+01 3.641e-20
1.550e+01 6.241e-20
1.600e+01 9.206e-20
1.650e+01 1.362e-19
1.700e+01 1.73e-19
1.750e+01 2.081e-19
1.800e+01 2.479e-19
1.850e+01 2.88e-19
1.900e+01 3.28e-19
1.950e+01 3.676e-19
2.000e+01 4.058e-19
2.100e+01 4.797e-19
2.200e+01 5.499e-19
2.300e+01 6.162e-19
2.400e+01 6.789e-19
2.500e+01 7.381e-19
2.600e+01 7.939e-19
2.700e+01 8.467e-19
2.800e+01 8.965e-19
2.900e+01 9.436e-19
3.000e+01 9.881e-19
3.500e+01 1.177e-18
4.000e+01 1.319e-18
4.500e+01 1.426e-18
5.000e+01 1.507e-18
6.000e+01 1.609e-18
7.000e+01 1.659e-18
8.000e+01 1.674e-18
9.000e+01 1.668e-18
1.000e+02 1.648e-18
1.250e+02 1.567e-18
1.500e+02 1.47e-18
2.000e+02 1.284e-18
2.500e+02 1.13e-18
3.000e+02 1.007e-18
3.500e+02 9.091e-19
4.000e+02 8.293e-19
4.500e+02 7.624e-19
5.000e+02 7.046e-19