{"qid": "D3109", "reaction": "e- + H2 X(1\u03a3+g);v=13 \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": 10.2985, "fit": {"coeffs": {"A1": 0.16344, "A2": -0.51929, "A3": 3.8879, "A4": -6.9578, "A5": 5.2193}, "func": "singlet_triplet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:31.672794+00:00"} ------------------------------------------------------------------------ 1.030e+01 0.0 1.050e+01 1.209e-18 1.150e+01 2.761e-18 1.200e+01 2.942e-18 1.250e+01 2.952e-18 1.300e+01 2.873e-18 1.350e+01 2.753e-18 1.400e+01 2.637e-18 1.450e+01 2.59e-18 1.500e+01 2.481e-18 1.550e+01 2.357e-18 1.600e+01 2.232e-18 1.650e+01 2.136e-18 1.700e+01 2.029e-18 1.750e+01 1.925e-18 1.800e+01 1.837e-18 1.850e+01 1.745e-18 1.900e+01 1.657e-18 1.950e+01 1.572e-18 2.000e+01 1.493e-18 2.100e+01 1.346e-18 2.200e+01 1.216e-18 2.300e+01 1.1e-18 2.400e+01 9.975e-19 2.500e+01 9.067e-19 2.600e+01 8.26e-19 2.700e+01 7.543e-19 2.800e+01 6.905e-19 2.900e+01 6.334e-19 3.000e+01 5.824e-19 3.500e+01 3.945e-19 4.000e+01 2.793e-19 4.500e+01 2.05e-19 5.000e+01 1.549e-19 6.000e+01 9.481e-20 7.000e+01 6.236e-20 8.000e+01 4.327e-20 9.000e+01 3.128e-20 1.000e+02 2.337e-20 1.250e+02 1.255e-20 1.500e+02 7.53e-21