{"qid": "D2289", "reaction": "e- + D2 X(1\u03a3+g);v=10 \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": 13.5838, "fit": {"coeffs": {"A1": 0.43838, "A2": 0.42028, "A3": -2.5895, "A4": 5.9194, "A5": -5.9728, "A6": 2.2391}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:44.491572+00:00"} ------------------------------------------------------------------------ 1.358e+01 0.0 1.400e+01 5.488e-21 1.450e+01 1.79e-20 1.500e+01 4.067e-20 1.550e+01 6.971e-20 1.600e+01 1.085e-19 1.650e+01 1.434e-19 1.700e+01 1.815e-19 1.750e+01 2.201e-19 1.800e+01 2.637e-19 1.850e+01 3.075e-19 1.900e+01 3.509e-19 1.950e+01 3.939e-19 2.000e+01 4.353e-19 2.100e+01 5.158e-19 2.200e+01 5.919e-19 2.300e+01 6.64e-19 2.400e+01 7.323e-19 2.500e+01 7.967e-19 2.600e+01 8.576e-19 2.700e+01 9.151e-19 2.800e+01 9.694e-19 2.900e+01 1.021e-18 3.000e+01 1.069e-18 3.500e+01 1.276e-18 4.000e+01 1.432e-18 4.500e+01 1.55e-18 5.000e+01 1.639e-18 6.000e+01 1.753e-18 7.000e+01 1.809e-18 8.000e+01 1.827e-18 9.000e+01 1.822e-18 1.000e+02 1.801e-18 1.250e+02 1.714e-18 1.500e+02 1.608e-18 2.000e+02 1.403e-18 2.500e+02 1.233e-18 3.000e+02 1.099e-18 3.500e+02 9.913e-19 4.000e+02 9.041e-19 4.500e+02 8.315e-19 5.000e+02 7.689e-19