{"qid": "D2226", "reaction": "e- + D2 X(1\u03a3+g);v=12 \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": 11.2535, "fit": {"coeffs": {"A1": 0.65928, "A2": 0.57359, "A3": -2.5849, "A4": 5.2102, "A5": -4.0648, "A6": 1.083}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:27.315479+00:00"}
------------------------------------------------------------------------
1.125e+01 0.0
1.150e+01 9.114e-20
1.200e+01 3.298e-19
1.250e+01 6.351e-19
1.300e+01 9.362e-19
1.350e+01 1.16e-18
1.400e+01 1.339e-18
1.450e+01 1.514e-18
1.500e+01 1.679e-18
1.550e+01 1.823e-18
1.600e+01 1.959e-18
1.650e+01 2.085e-18
1.700e+01 2.202e-18
1.750e+01 2.311e-18
1.800e+01 2.413e-18
1.850e+01 2.51e-18
1.900e+01 2.602e-18
1.950e+01 2.688e-18
2.000e+01 2.77e-18
2.100e+01 2.92e-18
2.200e+01 3.056e-18
2.300e+01 3.177e-18
2.400e+01 3.287e-18
2.500e+01 3.386e-18
2.600e+01 3.475e-18
2.700e+01 3.556e-18
2.800e+01 3.629e-18
2.900e+01 3.695e-18
3.000e+01 3.754e-18
3.500e+01 3.974e-18
4.000e+01 4.097e-18
4.500e+01 4.158e-18
5.000e+01 4.175e-18
6.000e+01 4.133e-18
7.000e+01 4.033e-18
8.000e+01 3.906e-18
9.000e+01 3.769e-18
1.000e+02 3.631e-18
1.250e+02 3.302e-18
1.500e+02 3.011e-18
2.000e+02 2.545e-18
2.500e+02 2.198e-18
3.000e+02 1.932e-18
3.500e+02 1.723e-18
4.000e+02 1.555e-18
4.500e+02 1.416e-18
5.000e+02 1.3e-18