{"qid": "D3161", "reaction": "e- + H2 X(1\u03a3+g);v=7 \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": 11.6693, "fit": {"coeffs": {"A1": 0.16249, "A2": 0.03403, "A3": 0.1313, "A4": -0.20561, "A5": 0.25058, "A6": -0.18428}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:46.188872+00:00"} ------------------------------------------------------------------------ 1.167e+01 0.0 1.200e+01 8.317e-21 1.250e+01 5.058e-20 1.300e+01 1.145e-19 1.350e+01 1.906e-19 1.400e+01 2.58e-19 1.450e+01 3.358e-19 1.500e+01 3.527e-19 1.550e+01 3.735e-19 1.600e+01 3.936e-19 1.650e+01 4.212e-19 1.700e+01 4.325e-19 1.750e+01 4.68e-19 1.800e+01 5.037e-19 1.850e+01 5.306e-19 1.900e+01 5.496e-19 1.950e+01 5.638e-19 2.000e+01 5.744e-19 2.100e+01 5.888e-19 2.200e+01 5.978e-19 2.300e+01 6.04e-19 2.400e+01 6.081e-19 2.500e+01 6.1e-19 2.600e+01 6.103e-19 2.700e+01 6.093e-19 2.800e+01 6.07e-19 2.900e+01 6.036e-19 3.000e+01 5.993e-19 3.500e+01 5.677e-19 4.000e+01 5.311e-19 4.500e+01 4.962e-19 5.000e+01 4.654e-19 6.000e+01 4.16e-19 7.000e+01 3.786e-19 8.000e+01 3.491e-19 9.000e+01 3.248e-19 1.000e+02 3.041e-19 1.250e+02 2.626e-19 1.500e+02 2.31e-19 2.000e+02 1.862e-19 2.500e+02 1.559e-19 3.000e+02 1.325e-19 3.500e+02 1.122e-19 4.000e+02 9.469e-20 4.500e+02 8.249e-20 5.000e+02 8.094e-20