{"qid": "D2273", "reaction": "e- + D2 X(1\u03a3+g);v=15 \u2192 D2 c(3\u03a0u) + 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": 10.7142, "fit": {"coeffs": {"A1": -3.3588e-06, "A2": 0.10719, "A3": 0.17476, "A4": 2.5783, "A5": -2.9012}, "func": "singlet_triplet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:40.107548+00:00"} ------------------------------------------------------------------------ 1.071e+01 0.0 1.150e+01 2.617e-19 1.200e+01 5.879e-19 1.250e+01 9.336e-19 1.300e+01 1.309e-18 1.350e+01 1.591e-18 1.400e+01 1.827e-18 1.450e+01 1.862e-18 1.500e+01 1.972e-18 1.550e+01 2.003e-18 1.600e+01 2.104e-18 1.650e+01 2.144e-18 1.700e+01 2.141e-18 1.750e+01 2.115e-18 1.800e+01 2.073e-18 1.850e+01 2.019e-18 1.900e+01 1.959e-18 1.950e+01 1.897e-18 2.000e+01 1.832e-18 2.100e+01 1.702e-18 2.200e+01 1.575e-18 2.300e+01 1.456e-18 2.400e+01 1.344e-18 2.500e+01 1.242e-18 2.600e+01 1.148e-18 2.700e+01 1.061e-18 2.800e+01 9.827e-19 2.900e+01 9.111e-19 3.000e+01 8.457e-19 3.500e+01 5.952e-19 4.000e+01 4.331e-19 4.500e+01 3.246e-19 5.000e+01 2.495e-19 6.000e+01 1.568e-19 7.000e+01 1.051e-19 8.000e+01 7.397e-20 9.000e+01 5.407e-20 1.000e+02 4.076e-20 1.250e+02 2.229e-20 1.500e+02 1.355e-20