{"qid": "D2207", "reaction": "e- + D2 X(1\u03a3+g);v=15 \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": 0.50991, "fit": {"coeffs": {"A1": 95400.0, "A2": 2.54, "A3": 9.6, "A4": 0.42}, "func": "EDE_b3Su"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:22.135451+00:00"} ------------------------------------------------------------------------ 5.099e-01 0.0 1.000e+00 3.866e-16 1.500e+00 3.337e-16 2.000e+00 2.589e-16 2.500e+00 2.282e-16 3.000e+00 2.113e-16 3.500e+00 2.003e-16 4.000e+00 1.934e-16 4.500e+00 1.852e-16 5.000e+00 1.778e-16 5.500e+00 1.719e-16 6.000e+00 1.661e-16 6.500e+00 1.594e-16 7.000e+00 1.522e-16 7.500e+00 1.447e-16 8.000e+00 1.37e-16 8.500e+00 1.298e-16 9.000e+00 1.225e-16 9.500e+00 1.143e-16 1.000e+01 1.06e-16 1.050e+01 9.802e-17 1.100e+01 9.078e-17 1.150e+01 8.53e-17 1.200e+01 8.056e-17 1.250e+01 7.571e-17 1.300e+01 7.12e-17 1.350e+01 6.727e-17 1.400e+01 6.373e-17 1.450e+01 6.044e-17 1.500e+01 5.74e-17 1.550e+01 5.444e-17 1.600e+01 5.155e-17 1.650e+01 4.881e-17 1.700e+01 4.63e-17 1.750e+01 4.399e-17 1.800e+01 4.179e-17 1.850e+01 3.972e-17 1.900e+01 3.78e-17 1.950e+01 3.606e-17 2.000e+01 3.45e-17 2.100e+01 3.171e-17 2.200e+01 2.918e-17 2.300e+01 2.688e-17 2.400e+01 2.48e-17 2.500e+01 2.29e-17 2.600e+01 2.117e-17 2.700e+01 1.957e-17 2.800e+01 1.809e-17 2.900e+01 1.67e-17 3.000e+01 1.538e-17 3.500e+01 1.091e-17 4.000e+01 8.583e-18 4.500e+01 6.837e-18 5.000e+01 5.798e-18 6.000e+01 4.434e-18 7.000e+01 3.115e-18 8.000e+01 2.22e-18 9.000e+01 1.594e-18 1.000e+02 1.168e-18 1.250e+02 6.059e-19 1.500e+02 3.235e-19