{"qid": "D2298", "reaction": "e- + D2 X(1\u03a3+g);v=18 \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": 12.236, "fit": {"coeffs": {"A1": 0.35989, "A2": 0.30887, "A3": -1.9688, "A4": 4.56, "A5": -4.624, "A6": 1.7411}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:46.939585+00:00"}
------------------------------------------------------------------------
1.224e+01 0.0
1.250e+01 1.587e-21
1.300e+01 1.013e-20
1.350e+01 2.818e-20
1.400e+01 5.393e-20
1.450e+01 8.265e-20
1.500e+01 1.133e-19
1.550e+01 1.417e-19
1.600e+01 1.691e-19
1.650e+01 1.982e-19
1.700e+01 2.263e-19
1.750e+01 2.545e-19
1.800e+01 2.825e-19
1.850e+01 3.104e-19
1.900e+01 3.381e-19
1.950e+01 3.654e-19
2.000e+01 3.916e-19
2.100e+01 4.421e-19
2.200e+01 4.899e-19
2.300e+01 5.35e-19
2.400e+01 5.774e-19
2.500e+01 6.174e-19
2.600e+01 6.551e-19
2.700e+01 6.906e-19
2.800e+01 7.242e-19
2.900e+01 7.559e-19
3.000e+01 7.858e-19
3.500e+01 9.126e-19
4.000e+01 1.008e-18
4.500e+01 1.08e-18
5.000e+01 1.134e-18
6.000e+01 1.201e-18
7.000e+01 1.231e-18
8.000e+01 1.238e-18
9.000e+01 1.229e-18
1.000e+02 1.211e-18
1.250e+02 1.143e-18
1.500e+02 1.064e-18
2.000e+02 9.168e-19
2.500e+02 7.984e-19
3.000e+02 7.071e-19
3.500e+02 6.362e-19
4.000e+02 5.799e-19
4.500e+02 5.334e-19
5.000e+02 4.933e-19