{"qid": "D2306", "reaction": "e- + D2 X(1\u03a3+g);v=6 \u2192 D2 D(1\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": 14.6399, "fit": {"coeffs": {"A1": 0.38638, "A2": 0.33056, "A3": -1.8776, "A4": 4.0717, "A5": -3.9068, "A6": 1.3786}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:49.155597+00:00"} ------------------------------------------------------------------------ 1.464e+01 0.0 1.500e+01 1.283e-21 1.550e+01 5.818e-21 1.600e+01 1.797e-20 1.650e+01 3.423e-20 1.700e+01 5.678e-20 1.750e+01 8.974e-20 1.800e+01 1.252e-19 1.850e+01 1.609e-19 1.900e+01 1.965e-19 1.950e+01 2.315e-19 2.000e+01 2.665e-19 2.100e+01 3.34e-19 2.200e+01 3.982e-19 2.300e+01 4.594e-19 2.400e+01 5.176e-19 2.500e+01 5.727e-19 2.600e+01 6.249e-19 2.700e+01 6.744e-19 2.800e+01 7.212e-19 2.900e+01 7.656e-19 3.000e+01 8.077e-19 3.500e+01 9.87e-19 4.000e+01 1.124e-18 4.500e+01 1.228e-18 5.000e+01 1.306e-18 6.000e+01 1.408e-18 7.000e+01 1.46e-18 8.000e+01 1.479e-18 9.000e+01 1.478e-18 1.000e+02 1.464e-18 1.250e+02 1.397e-18 1.500e+02 1.314e-18 2.000e+02 1.152e-18 2.500e+02 1.017e-18 3.000e+02 9.083e-19 3.500e+02 8.21e-19 4.000e+02 7.496e-19 4.500e+02 6.893e-19 5.000e+02 6.368e-19