{"qid": "D3123", "reaction": "e- + H2 X(1\u03a3+g);v=12 \u2192 H2 EF(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": 10.4282, "fit": {"coeffs": {"A1": 2.4878e-05, "A2": 0.44189, "A3": -1.9308, "A4": 4.3538, "A5": -3.5713, "A6": 0.55592}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:35.596815+00:00"} ------------------------------------------------------------------------ 1.043e+01 0.0 1.050e+01 8.031e-22 1.150e+01 3.955e-20 1.200e+01 7.838e-20 1.250e+01 1.673e-19 1.300e+01 3.164e-19 1.350e+01 4.765e-19 1.400e+01 6.872e-19 1.450e+01 7.136e-19 1.500e+01 7.566e-19 1.550e+01 7.939e-19 1.600e+01 8.854e-19 1.650e+01 9.681e-19 1.700e+01 1.047e-18 1.750e+01 1.067e-18 1.800e+01 1.077e-18 1.850e+01 1.082e-18 1.900e+01 1.084e-18 1.950e+01 1.079e-18 2.000e+01 1.075e-18 2.100e+01 1.068e-18 2.200e+01 1.06e-18 2.300e+01 1.048e-18 2.400e+01 1.033e-18 2.500e+01 1.02e-18 2.600e+01 1.007e-18 2.700e+01 9.953e-19 2.800e+01 9.846e-19 2.900e+01 9.753e-19 3.000e+01 9.682e-19 3.500e+01 9.441e-19 4.000e+01 9.348e-19 4.500e+01 9.372e-19 5.000e+01 9.382e-19 6.000e+01 9.216e-19 7.000e+01 8.694e-19 8.000e+01 8.203e-19 9.000e+01 7.784e-19 1.000e+02 7.415e-19 1.250e+02 6.66e-19 1.500e+02 6.031e-19 2.000e+02 4.97e-19 2.500e+02 3.973e-19 3.000e+02 3.19e-19 3.500e+02 2.765e-19 4.000e+02 2.497e-19 4.500e+02 2.238e-19 5.000e+02 2.043e-19