{"qid": "D3150", "reaction": "e- + H2 X(1\u03a3+g);v=10 \u2192 H2 GK(1\u03a3+g) + 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": 10.8187, "fit": {"coeffs": {"A1": 0.20111, "A2": 0.095449, "A3": 0.14977, "A4": -0.49293, "A5": 0.9818, "A6": -0.67169}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:43.200856+00:00"}
------------------------------------------------------------------------
1.082e+01 0.0
1.150e+01 9.22e-20
1.200e+01 2.263e-19
1.250e+01 4.152e-19
1.300e+01 5.607e-19
1.350e+01 6.484e-19
1.400e+01 7.087e-19
1.450e+01 7.666e-19
1.500e+01 8.36e-19
1.550e+01 8.669e-19
1.600e+01 8.972e-19
1.650e+01 9.327e-19
1.700e+01 9.585e-19
1.750e+01 9.831e-19
1.800e+01 1.013e-18
1.850e+01 1.041e-18
1.900e+01 1.061e-18
1.950e+01 1.076e-18
2.000e+01 1.088e-18
2.100e+01 1.102e-18
2.200e+01 1.107e-18
2.300e+01 1.107e-18
2.400e+01 1.104e-18
2.500e+01 1.097e-18
2.600e+01 1.088e-18
2.700e+01 1.077e-18
2.800e+01 1.066e-18
2.900e+01 1.054e-18
3.000e+01 1.041e-18
3.500e+01 9.75e-19
4.000e+01 9.142e-19
4.500e+01 8.609e-19
5.000e+01 8.147e-19
6.000e+01 7.39e-19
7.000e+01 6.784e-19
8.000e+01 6.277e-19
9.000e+01 5.84e-19
1.000e+02 5.457e-19
1.250e+02 4.673e-19
1.500e+02 4.073e-19
2.000e+02 3.236e-19
2.500e+02 2.688e-19
3.000e+02 2.284e-19
3.500e+02 1.949e-19
4.000e+02 1.666e-19
4.500e+02 1.457e-19
5.000e+02 1.385e-19