{"qid": "D3154", "reaction": "e- + H2 X(1\u03a3+g);v=13 \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": 10.2985, "fit": {"coeffs": {"A1": -9.181e-05, "A2": 0.21733, "A3": -0.81289, "A4": 2.5142, "A5": -3.104, "A6": 1.2906}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:44.284862+00:00"} ------------------------------------------------------------------------ 1.030e+01 0.0 1.050e+01 8.475e-20 1.150e+01 2.371e-19 1.200e+01 3.635e-19 1.250e+01 4.868e-19 1.300e+01 5.596e-19 1.350e+01 6.095e-19 1.400e+01 6.668e-19 1.450e+01 7.317e-19 1.500e+01 7.598e-19 1.550e+01 7.908e-19 1.600e+01 8.207e-19 1.650e+01 8.437e-19 1.700e+01 8.661e-19 1.750e+01 8.817e-19 1.800e+01 8.979e-19 1.850e+01 9.129e-19 1.900e+01 9.234e-19 1.950e+01 9.3e-19 2.000e+01 9.334e-19 2.100e+01 9.33e-19 2.200e+01 9.256e-19 2.300e+01 9.136e-19 2.400e+01 8.988e-19 2.500e+01 8.823e-19 2.600e+01 8.65e-19 2.700e+01 8.475e-19 2.800e+01 8.301e-19 2.900e+01 8.131e-19 3.000e+01 7.967e-19 3.500e+01 7.257e-19 4.000e+01 6.719e-19 4.500e+01 6.307e-19 5.000e+01 5.98e-19 6.000e+01 5.474e-19 7.000e+01 5.075e-19 8.000e+01 4.73e-19 9.000e+01 4.422e-19 1.000e+02 4.142e-19 1.250e+02 3.547e-19 1.500e+02 3.083e-19 2.000e+02 2.449e-19 2.500e+02 2.061e-19 3.000e+02 1.786e-19 3.500e+02 1.548e-19 4.000e+02 1.324e-19 4.500e+02 1.141e-19 5.000e+02 1.076e-19