{"qid": "D2160", "reaction": "e- + D2 X(1\u03a3+g);v=12 \u2192 D2 a(3\u03a3+g) + 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": 11.2535, "fit": {"coeffs": {"A1": 1.8509e-07, "A2": 0.11873, "A3": -1.0732, "A4": 4.7343, "A5": -3.6516}, "func": "singlet_triplet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:09.003380+00:00"} ------------------------------------------------------------------------ 1.125e+01 0.0 1.150e+01 8.261e-20 1.200e+01 3.046e-19 1.250e+01 6.898e-19 1.300e+01 1.119e-18 1.350e+01 1.571e-18 1.400e+01 1.734e-18 1.450e+01 1.848e-18 1.500e+01 1.843e-18 1.550e+01 1.778e-18 1.600e+01 1.723e-18 1.650e+01 1.693e-18 1.700e+01 1.664e-18 1.750e+01 1.661e-18 1.800e+01 1.606e-18 1.850e+01 1.555e-18 1.900e+01 1.499e-18 1.950e+01 1.438e-18 2.000e+01 1.374e-18 2.100e+01 1.24e-18 2.200e+01 1.112e-18 2.300e+01 9.959e-19 2.400e+01 8.914e-19 2.500e+01 7.987e-19 2.600e+01 7.169e-19 2.700e+01 6.449e-19 2.800e+01 5.816e-19 2.900e+01 5.257e-19 3.000e+01 4.764e-19 3.500e+01 3.016e-19 4.000e+01 2.019e-19 4.500e+01 1.42e-19 5.000e+01 1.037e-19 6.000e+01 6.015e-20 7.000e+01 3.793e-20 8.000e+01 2.544e-20 9.000e+01 1.788e-20 1.000e+02 1.304e-20 1.250e+02 6.683e-21 1.500e+02 3.869e-21