{"qid": "D2299", "reaction": "e- + D2 X(1\u03a3+g);v=19 \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": 12.1598, "fit": {"coeffs": {"A1": 0.31323, "A2": 0.23324, "A3": -1.4868, "A4": 3.4419, "A5": -3.4826, "A6": 1.3075}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:47.207587+00:00"} ------------------------------------------------------------------------ 1.216e+01 0.0 1.250e+01 2.049e-21 1.300e+01 9.643e-21 1.350e+01 2.534e-20 1.400e+01 4.672e-20 1.450e+01 7.001e-20 1.500e+01 9.38e-20 1.550e+01 1.15e-19 1.600e+01 1.353e-19 1.650e+01 1.583e-19 1.700e+01 1.796e-19 1.750e+01 2.011e-19 1.800e+01 2.222e-19 1.850e+01 2.434e-19 1.900e+01 2.643e-19 1.950e+01 2.849e-19 2.000e+01 3.046e-19 2.100e+01 3.426e-19 2.200e+01 3.785e-19 2.300e+01 4.123e-19 2.400e+01 4.442e-19 2.500e+01 4.742e-19 2.600e+01 5.025e-19 2.700e+01 5.291e-19 2.800e+01 5.543e-19 2.900e+01 5.78e-19 3.000e+01 6.004e-19 3.500e+01 6.953e-19 4.000e+01 7.667e-19 4.500e+01 8.203e-19 5.000e+01 8.603e-19 6.000e+01 9.099e-19 7.000e+01 9.321e-19 8.000e+01 9.366e-19 9.000e+01 9.297e-19 1.000e+02 9.153e-19 1.250e+02 8.631e-19 1.500e+02 8.032e-19 2.000e+02 6.913e-19 2.500e+02 6.016e-19 3.000e+02 5.325e-19 3.500e+02 4.792e-19 4.000e+02 4.368e-19 4.500e+02 4.018e-19 5.000e+02 3.715e-19