{"qid": "D2229", "reaction": "e- + D2 X(1\u03a3+g);v=15 \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": 10.7142, "fit": {"coeffs": {"A1": 0.55945, "A2": 0.87897, "A3": -3.7363, "A4": 8.5676, "A5": -8.9351, "A6": 3.8213}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:28.151484+00:00"} ------------------------------------------------------------------------ 1.071e+01 0.0 1.150e+01 8.496e-19 1.200e+01 1.294e-18 1.250e+01 1.593e-18 1.300e+01 1.801e-18 1.350e+01 1.971e-18 1.400e+01 2.15e-18 1.450e+01 2.306e-18 1.500e+01 2.428e-18 1.550e+01 2.551e-18 1.600e+01 2.661e-18 1.650e+01 2.761e-18 1.700e+01 2.853e-18 1.750e+01 2.939e-18 1.800e+01 3.018e-18 1.850e+01 3.092e-18 1.900e+01 3.161e-18 1.950e+01 3.226e-18 2.000e+01 3.286e-18 2.100e+01 3.397e-18 2.200e+01 3.494e-18 2.300e+01 3.58e-18 2.400e+01 3.657e-18 2.500e+01 3.724e-18 2.600e+01 3.784e-18 2.700e+01 3.837e-18 2.800e+01 3.883e-18 2.900e+01 3.925e-18 3.000e+01 3.961e-18 3.500e+01 4.081e-18 4.000e+01 4.13e-18 4.500e+01 4.132e-18 5.000e+01 4.105e-18 6.000e+01 3.997e-18 7.000e+01 3.856e-18 8.000e+01 3.703e-18 9.000e+01 3.549e-18 1.000e+02 3.4e-18 1.250e+02 3.059e-18 1.500e+02 2.769e-18 2.000e+02 2.316e-18 2.500e+02 1.986e-18 3.000e+02 1.736e-18 3.500e+02 1.542e-18 4.000e+02 1.386e-18 4.500e+02 1.259e-18 5.000e+02 1.153e-18