{"qid": "D3065", "reaction": "e- + H2 X(1\u03a3+g);v=14 \u2192 H2 c(3\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": 10.2218, "fit": {"coeffs": {"A1": -2.0288e-06, "A2": 0.029119, "A3": 0.058126, "A4": 0.71753, "A5": -0.81075}, "func": "singlet_triplet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:19.452728+00:00"}
------------------------------------------------------------------------
1.022e+01 0.0
1.050e+01 1.391e-20
1.150e+01 1.792e-19
1.200e+01 2.745e-19
1.250e+01 3.723e-19
1.300e+01 4.992e-19
1.350e+01 5.664e-19
1.400e+01 5.999e-19
1.450e+01 5.866e-19
1.500e+01 5.898e-19
1.550e+01 5.867e-19
1.600e+01 5.994e-19
1.650e+01 6.013e-19
1.700e+01 5.934e-19
1.750e+01 5.806e-19
1.800e+01 5.645e-19
1.850e+01 5.464e-19
1.900e+01 5.276e-19
1.950e+01 5.082e-19
2.000e+01 4.887e-19
2.100e+01 4.507e-19
2.200e+01 4.148e-19
2.300e+01 3.814e-19
2.400e+01 3.508e-19
2.500e+01 3.228e-19
2.600e+01 2.974e-19
2.700e+01 2.743e-19
2.800e+01 2.533e-19
2.900e+01 2.343e-19
3.000e+01 2.171e-19
3.500e+01 1.517e-19
4.000e+01 1.098e-19
4.500e+01 8.197e-20
5.000e+01 6.282e-20
6.000e+01 3.93e-20
7.000e+01 2.625e-20
8.000e+01 1.843e-20
9.000e+01 1.345e-20
1.000e+02 1.013e-20
1.250e+02 5.522e-21
1.500e+02 3.35e-21