{"qid": "D3056", "reaction": "e- + H2 X(1\u03a3+g);v=7 \u2192 H2 C(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": 11.6693, "fit": {"coeffs": {"A1": 1.1372, "A2": 1.2483, "A3": -10.821, "A4": 27.365, "A5": -28.762, "A6": 10.996}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:16.996715+00:00"} ------------------------------------------------------------------------ 1.167e+01 0.0 1.200e+01 8.972e-21 1.250e+01 6.118e-20 1.300e+01 1.355e-19 1.350e+01 2.775e-19 1.400e+01 4.464e-19 1.450e+01 7.733e-19 1.500e+01 1.032e-18 1.550e+01 1.262e-18 1.600e+01 1.524e-18 1.650e+01 1.791e-18 1.700e+01 2.05e-18 1.750e+01 2.302e-18 1.800e+01 2.544e-18 1.850e+01 2.779e-18 1.900e+01 3.005e-18 1.950e+01 3.223e-18 2.000e+01 3.433e-18 2.100e+01 3.832e-18 2.200e+01 4.203e-18 2.300e+01 4.55e-18 2.400e+01 4.873e-18 2.500e+01 5.176e-18 2.600e+01 5.458e-18 2.700e+01 5.723e-18 2.800e+01 5.97e-18 2.900e+01 6.202e-18 3.000e+01 6.42e-18 3.500e+01 7.322e-18 4.000e+01 7.977e-18 4.500e+01 8.45e-18 5.000e+01 8.785e-18 6.000e+01 9.164e-18 7.000e+01 9.29e-18 8.000e+01 9.262e-18 9.000e+01 9.14e-18 1.000e+02 8.96e-18 1.250e+02 8.399e-18 1.500e+02 7.807e-18 2.000e+02 6.751e-18 2.500e+02 5.923e-18 3.000e+02 5.284e-18 3.500e+02 4.782e-18 4.000e+02 4.374e-18 4.500e+02 4.027e-18 5.000e+02 3.717e-18