{"qid": "D2302", "reaction": "e- + D2 X(1\u03a3+g);v=2 \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": 15.9218, "fit": {"coeffs": {"A1": 0.26233, "A2": 0.14824, "A3": -0.73862, "A4": 1.462, "A5": -1.2646, "A6": 0.3989}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:48.023591+00:00"} ------------------------------------------------------------------------ 1.592e+01 0.0 1.600e+01 9.903e-23 1.650e+01 4.712e-21 1.700e+01 1.621e-20 1.750e+01 3.097e-20 1.800e+01 4.703e-20 1.850e+01 6.367e-20 1.900e+01 8.045e-20 1.950e+01 9.711e-20 2.000e+01 1.138e-19 2.100e+01 1.463e-19 2.200e+01 1.777e-19 2.300e+01 2.075e-19 2.400e+01 2.358e-19 2.500e+01 2.628e-19 2.600e+01 2.886e-19 2.700e+01 3.13e-19 2.800e+01 3.361e-19 2.900e+01 3.581e-19 3.000e+01 3.789e-19 3.500e+01 4.681e-19 4.000e+01 5.363e-19 4.500e+01 5.883e-19 5.000e+01 6.278e-19 6.000e+01 6.794e-19 7.000e+01 7.058e-19 8.000e+01 7.161e-19 9.000e+01 7.161e-19 1.000e+02 7.096e-19 1.250e+02 6.782e-19 1.500e+02 6.385e-19 2.000e+02 5.608e-19 2.500e+02 4.956e-19 3.000e+02 4.432e-19 3.500e+02 4.011e-19 4.000e+02 3.663e-19 4.500e+02 3.37e-19 5.000e+02 3.114e-19