{"qid": "D3108", "reaction": "e- + H2 X(1\u03a3+g);v=12 \u2192 H2 e(3\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": 10.4282, "fit": {"coeffs": {"A1": 6.2312e-06, "A2": 0.045013, "A3": -0.038133, "A4": 1.0197, "A5": -1.0226}, "func": "singlet_triplet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:31.392792+00:00"} ------------------------------------------------------------------------ 1.043e+01 0.0 1.050e+01 3.81e-22 1.150e+01 2.864e-19 1.200e+01 3.858e-19 1.250e+01 4.619e-19 1.300e+01 5.162e-19 1.350e+01 6.171e-19 1.400e+01 6.429e-19 1.450e+01 6.421e-19 1.500e+01 6.42e-19 1.550e+01 6.907e-19 1.600e+01 6.589e-19 1.650e+01 6.673e-19 1.700e+01 6.543e-19 1.750e+01 6.403e-19 1.800e+01 6.4e-19 1.850e+01 6.261e-19 1.900e+01 6.08e-19 1.950e+01 5.881e-19 2.000e+01 5.694e-19 2.100e+01 5.298e-19 2.200e+01 4.903e-19 2.300e+01 4.525e-19 2.400e+01 4.172e-19 2.500e+01 3.845e-19 2.600e+01 3.545e-19 2.700e+01 3.271e-19 2.800e+01 3.021e-19 2.900e+01 2.795e-19 3.000e+01 2.588e-19 3.500e+01 1.802e-19 4.000e+01 1.299e-19 4.500e+01 9.661e-20 5.000e+01 7.374e-20 6.000e+01 4.579e-20 7.000e+01 3.042e-20 8.000e+01 2.127e-20 9.000e+01 1.547e-20 1.000e+02 1.162e-20 1.250e+02 6.295e-21 1.500e+02 3.799e-21