{"qid": "D2282", "reaction": "e- + D2 X(1\u03a3+g);v=4 \u2192 D2 c(3\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": 13.3627, "fit": {"coeffs": {"A1": -4.5792e-06, "A2": 0.31958, "A3": -2.142, "A4": 6.883, "A5": -4.9424}, "func": "singlet_triplet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:42.543561+00:00"}
------------------------------------------------------------------------
1.336e+01 0.0
1.350e+01 1.369e-20
1.400e+01 1.547e-19
1.450e+01 6.885e-19
1.500e+01 1.305e-18
1.550e+01 1.632e-18
1.600e+01 1.823e-18
1.650e+01 1.934e-18
1.700e+01 1.993e-18
1.750e+01 2.015e-18
1.800e+01 2.014e-18
1.850e+01 1.993e-18
1.900e+01 1.96e-18
1.950e+01 1.918e-18
2.000e+01 1.871e-18
2.100e+01 1.765e-18
2.200e+01 1.654e-18
2.300e+01 1.543e-18
2.400e+01 1.437e-18
2.500e+01 1.336e-18
2.600e+01 1.242e-18
2.700e+01 1.155e-18
2.800e+01 1.074e-18
2.900e+01 9.997e-19
3.000e+01 9.314e-19
3.500e+01 6.645e-19
4.000e+01 4.881e-19
4.500e+01 3.683e-19
5.000e+01 2.846e-19
6.000e+01 1.803e-19
7.000e+01 1.215e-19
8.000e+01 8.586e-20
9.000e+01 6.3e-20
1.000e+02 4.765e-20
1.250e+02 2.621e-20
1.500e+02 1.6e-20