{"qid": "D3125", "reaction": "e- + H2 X(1\u03a3+g);v=14 \u2192 H2 EF(1\u03a3+g) + 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": 10.2218, "fit": {"coeffs": {"A1": 5.5734e-05, "A2": 0.1662, "A3": -0.74065, "A4": 1.8137, "A5": -1.7292, "A6": 0.45504}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:36.160818+00:00"} ------------------------------------------------------------------------ 1.022e+01 0.0 1.050e+01 7.61e-21 1.150e+01 4.162e-20 1.200e+01 7.134e-20 1.250e+01 1.137e-19 1.300e+01 1.749e-19 1.350e+01 2.317e-19 1.400e+01 2.832e-19 1.450e+01 3.004e-19 1.500e+01 3.191e-19 1.550e+01 3.327e-19 1.600e+01 3.639e-19 1.650e+01 3.96e-19 1.700e+01 4.232e-19 1.750e+01 4.3e-19 1.800e+01 4.324e-19 1.850e+01 4.344e-19 1.900e+01 4.346e-19 1.950e+01 4.337e-19 2.000e+01 4.314e-19 2.100e+01 4.289e-19 2.200e+01 4.251e-19 2.300e+01 4.204e-19 2.400e+01 4.143e-19 2.500e+01 4.085e-19 2.600e+01 4.032e-19 2.700e+01 3.98e-19 2.800e+01 3.932e-19 2.900e+01 3.888e-19 3.000e+01 3.851e-19 3.500e+01 3.69e-19 4.000e+01 3.596e-19 4.500e+01 3.593e-19 5.000e+01 3.601e-19 6.000e+01 3.536e-19 7.000e+01 3.308e-19 8.000e+01 3.099e-19 9.000e+01 2.921e-19 1.000e+02 2.765e-19 1.250e+02 2.456e-19 1.500e+02 2.211e-19 2.000e+02 1.817e-19 2.500e+02 1.45e-19 3.000e+02 1.163e-19 3.500e+02 1.007e-19 4.000e+02 9.085e-20 4.500e+02 8.114e-20 5.000e+02 7.355e-20