{"qid": "D2231", "reaction": "e- + D2 X(1\u03a3+g);v=17 \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": 10.4473, "fit": {"coeffs": {"A1": 0.24718, "A2": 1.6681, "A3": -7.4379, "A4": 19.499, "A5": -24.794, "A6": 12.583}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:28.699487+00:00"}
------------------------------------------------------------------------
1.045e+01 0.0
1.050e+01 3.459e-19
1.150e+01 2.46e-18
1.200e+01 2.639e-18
1.250e+01 2.78e-18
1.300e+01 2.918e-18
1.350e+01 3.038e-18
1.400e+01 3.136e-18
1.450e+01 3.226e-18
1.500e+01 3.305e-18
1.550e+01 3.376e-18
1.600e+01 3.441e-18
1.650e+01 3.5e-18
1.700e+01 3.553e-18
1.750e+01 3.602e-18
1.800e+01 3.647e-18
1.850e+01 3.688e-18
1.900e+01 3.727e-18
1.950e+01 3.763e-18
2.000e+01 3.796e-18
2.100e+01 3.855e-18
2.200e+01 3.906e-18
2.300e+01 3.949e-18
2.400e+01 3.987e-18
2.500e+01 4.018e-18
2.600e+01 4.045e-18
2.700e+01 4.067e-18
2.800e+01 4.086e-18
2.900e+01 4.101e-18
3.000e+01 4.113e-18
3.500e+01 4.134e-18
4.000e+01 4.111e-18
4.500e+01 4.06e-18
5.000e+01 3.992e-18
6.000e+01 3.831e-18
7.000e+01 3.657e-18
8.000e+01 3.485e-18
9.000e+01 3.32e-18
1.000e+02 3.164e-18
1.250e+02 2.819e-18
1.500e+02 2.534e-18
2.000e+02 2.098e-18
2.500e+02 1.785e-18
3.000e+02 1.551e-18
3.500e+02 1.37e-18
4.000e+02 1.225e-18
4.500e+02 1.108e-18
5.000e+02 1.011e-18