{"qid": "D2209", "reaction": "e- + D2 X(1\u03a3+g);v=17 \u2192 D2 b(3\u03a3+u) + e-", "process_types": {"EDE": "Dissociative Excitation"}, "data_type": "cross section", "refs": {"B9": {"doi": "10.1016/j.adt.2020.101403"}}, "comment": "MCCC calculations of vibrationally-resolved electron-impact dissociative excitation of D2, 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": 0.242986, "fit": {"coeffs": {"A1": 111000000.0, "A2": 3.1, "A3": 16.2, "A4": 0.28}, "func": "EDE_b3Su"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:22.683454+00:00"} ------------------------------------------------------------------------ 2.430e-01 0.0 5.000e-01 2.783e-16 1.000e+00 6.697e-16 1.500e+00 5.387e-16 2.000e+00 3.581e-16 2.500e+00 2.979e-16 3.000e+00 2.723e-16 3.500e+00 2.508e-16 4.000e+00 2.37e-16 4.500e+00 2.24e-16 5.000e+00 2.131e-16 5.500e+00 2.036e-16 6.000e+00 1.949e-16 6.500e+00 1.862e-16 7.000e+00 1.771e-16 7.500e+00 1.669e-16 8.000e+00 1.567e-16 8.500e+00 1.477e-16 9.000e+00 1.388e-16 9.500e+00 1.287e-16 1.000e+01 1.186e-16 1.050e+01 1.094e-16 1.100e+01 1.013e-16 1.150e+01 9.489e-17 1.200e+01 8.941e-17 1.250e+01 8.411e-17 1.300e+01 7.929e-17 1.350e+01 7.515e-17 1.400e+01 7.136e-17 1.450e+01 6.761e-17 1.500e+01 6.408e-17 1.550e+01 6.079e-17 1.600e+01 5.763e-17 1.650e+01 5.465e-17 1.700e+01 5.188e-17 1.750e+01 4.928e-17 1.800e+01 4.678e-17 1.850e+01 4.441e-17 1.900e+01 4.221e-17 1.950e+01 4.02e-17 2.000e+01 3.843e-17 2.100e+01 3.53e-17 2.200e+01 3.248e-17 2.300e+01 2.994e-17 2.400e+01 2.764e-17 2.500e+01 2.556e-17 2.600e+01 2.367e-17 2.700e+01 2.194e-17 2.800e+01 2.033e-17 2.900e+01 1.882e-17 3.000e+01 1.737e-17 3.500e+01 1.248e-17 4.000e+01 9.923e-18 4.500e+01 7.959e-18 5.000e+01 6.748e-18 6.000e+01 5.106e-18 7.000e+01 3.549e-18 8.000e+01 2.485e-18 9.000e+01 1.76e-18 1.000e+02 1.279e-18 1.250e+02 6.671e-19 1.500e+02 3.498e-19