{"qid": "D2222", "reaction": "e- + D2 X(1\u03a3+g);v=0 \u2192 D2 B'(1\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": 14.76, "fit": {"coeffs": {"A1": 0.46469, "A2": 0.31909, "A3": -1.5139, "A4": 2.9729, "A5": -2.4479, "A6": 0.69762}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:26.207473+00:00"} ------------------------------------------------------------------------ 1.476e+01 0.0 1.500e+01 4.444e-21 1.550e+01 4.093e-20 1.600e+01 1.003e-19 1.650e+01 1.656e-19 1.700e+01 2.313e-19 1.750e+01 2.96e-19 1.800e+01 3.591e-19 1.850e+01 4.204e-19 1.900e+01 4.799e-19 1.950e+01 5.374e-19 2.000e+01 5.931e-19 2.100e+01 6.988e-19 2.200e+01 7.974e-19 2.300e+01 8.893e-19 2.400e+01 9.748e-19 2.500e+01 1.055e-18 2.600e+01 1.129e-18 2.700e+01 1.198e-18 2.800e+01 1.263e-18 2.900e+01 1.323e-18 3.000e+01 1.379e-18 3.500e+01 1.608e-18 4.000e+01 1.77e-18 4.500e+01 1.884e-18 5.000e+01 1.963e-18 6.000e+01 2.048e-18 7.000e+01 2.073e-18 8.000e+01 2.063e-18 9.000e+01 2.034e-18 1.000e+02 1.993e-18 1.250e+02 1.869e-18 1.500e+02 1.742e-18 2.000e+02 1.515e-18 2.500e+02 1.332e-18 3.000e+02 1.185e-18 3.500e+02 1.067e-18 4.000e+02 9.699e-19 4.500e+02 8.886e-19 5.000e+02 8.197e-19