{"qid": "D3079", "reaction": "e- + H2 X(1\u03a3+g);v=13 \u2192 H2 D(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": 12.1882, "fit": {"coeffs": {"A1": 0.32768, "A2": 0.2231, "A3": -1.4812, "A4": 3.4729, "A5": -3.5428, "A6": 1.3377}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:23.356749+00:00"} ------------------------------------------------------------------------ 1.219e+01 0.0 1.250e+01 7.238e-22 1.300e+01 6.294e-21 1.350e+01 1.813e-20 1.400e+01 3.466e-20 1.450e+01 5.605e-20 1.500e+01 7.934e-20 1.550e+01 1.024e-19 1.600e+01 1.279e-19 1.650e+01 1.494e-19 1.700e+01 1.716e-19 1.750e+01 1.931e-19 1.800e+01 2.154e-19 1.850e+01 2.376e-19 1.900e+01 2.597e-19 1.950e+01 2.814e-19 2.000e+01 3.022e-19 2.100e+01 3.424e-19 2.200e+01 3.804e-19 2.300e+01 4.162e-19 2.400e+01 4.498e-19 2.500e+01 4.815e-19 2.600e+01 5.114e-19 2.700e+01 5.396e-19 2.800e+01 5.661e-19 2.900e+01 5.912e-19 3.000e+01 6.148e-19 3.500e+01 7.147e-19 4.000e+01 7.898e-19 4.500e+01 8.461e-19 5.000e+01 8.877e-19 6.000e+01 9.398e-19 7.000e+01 9.63e-19 8.000e+01 9.677e-19 9.000e+01 9.608e-19 1.000e+02 9.462e-19 1.250e+02 8.932e-19 1.500e+02 8.323e-19 2.000e+02 7.186e-19 2.500e+02 6.269e-19 3.000e+02 5.558e-19 3.500e+02 5.003e-19 4.000e+02 4.56e-19 4.500e+02 4.194e-19 5.000e+02 3.878e-19