{"qid": "D3002", "reaction": "e- + H2 X(1\u03a3+g);v=1 \u2192 H2 B(1\u03a3+u) + 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": 14.1652, "fit": {"coeffs": {"A1": 0.2951, "A2": 0.2919, "A3": -1.4081, "A4": 2.9302, "A5": -2.8185, "A6": 1.0132}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:02.064635+00:00"} ------------------------------------------------------------------------ 1.417e+01 0.0 1.450e+01 2.205e-21 1.500e+01 1.305e-20 1.550e+01 3.085e-20 1.600e+01 5.329e-20 1.650e+01 7.895e-20 1.700e+01 1.066e-19 1.750e+01 1.353e-19 1.800e+01 1.643e-19 1.850e+01 1.933e-19 1.900e+01 2.22e-19 1.950e+01 2.502e-19 2.000e+01 2.779e-19 2.100e+01 3.315e-19 2.200e+01 3.826e-19 2.300e+01 4.309e-19 2.400e+01 4.763e-19 2.500e+01 5.191e-19 2.600e+01 5.593e-19 2.700e+01 5.97e-19 2.800e+01 6.322e-19 2.900e+01 6.653e-19 3.000e+01 6.962e-19 3.500e+01 8.234e-19 4.000e+01 9.147e-19 4.500e+01 9.802e-19 5.000e+01 1.026e-18 6.000e+01 1.078e-18 7.000e+01 1.097e-18 8.000e+01 1.097e-18 9.000e+01 1.085e-18 1.000e+02 1.067e-18 1.250e+02 1.007e-18 1.500e+02 9.411e-19 2.000e+02 8.166e-19 2.500e+02 7.118e-19 3.000e+02 6.263e-19 3.500e+02 5.577e-19 4.000e+02 5.041e-19 4.500e+02 4.635e-19 5.000e+02 4.348e-19