{"qid": "D3057", "reaction": "e- + H2 X(1\u03a3+g);v=8 \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": 11.3542, "fit": {"coeffs": {"A1": 1.1229, "A2": 1.1779, "A3": -10.782, "A4": 27.813, "A5": -29.813, "A6": 11.659}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:17.264717+00:00"} ------------------------------------------------------------------------ 1.135e+01 0.0 1.150e+01 8.64e-22 1.200e+01 1.911e-20 1.250e+01 8.842e-20 1.300e+01 2.114e-19 1.350e+01 3.764e-19 1.400e+01 5.624e-19 1.450e+01 8.259e-19 1.500e+01 1.088e-18 1.550e+01 1.306e-18 1.600e+01 1.55e-18 1.650e+01 1.801e-18 1.700e+01 2.046e-18 1.750e+01 2.283e-18 1.800e+01 2.511e-18 1.850e+01 2.732e-18 1.900e+01 2.945e-18 1.950e+01 3.15e-18 2.000e+01 3.347e-18 2.100e+01 3.722e-18 2.200e+01 4.072e-18 2.300e+01 4.397e-18 2.400e+01 4.701e-18 2.500e+01 4.985e-18 2.600e+01 5.251e-18 2.700e+01 5.499e-18 2.800e+01 5.732e-18 2.900e+01 5.95e-18 3.000e+01 6.154e-18 3.500e+01 7.001e-18 4.000e+01 7.617e-18 4.500e+01 8.061e-18 5.000e+01 8.375e-18 6.000e+01 8.733e-18 7.000e+01 8.852e-18 8.000e+01 8.824e-18 9.000e+01 8.707e-18 1.000e+02 8.534e-18 1.250e+02 7.996e-18 1.500e+02 7.427e-18 2.000e+02 6.413e-18 2.500e+02 5.619e-18 3.000e+02 5.01e-18 3.500e+02 4.533e-18 4.000e+02 4.146e-18 4.500e+02 3.817e-18 5.000e+02 3.522e-18