{"qid": "D3176", "reaction": "e- + H2 X(1\u03a3+g);v=7 \u2192 H2 H(1\u03a3+g) + e-", "process_types": {"EDE": "Dissociative Excitation"}, "data_type": "cross section", "refs": {"B10": {"doi": "10.1016/j.adt.2020.101361"}}, "comment": "MCCC calculations of vibrationally-resolved electron-impact dissociative excitation of H2, 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": 13.559, "fit": {"coeffs": {"A1": 0.085332, "A2": 0.042613, "A3": -0.1309, "A4": 0.48143, "A5": -0.61117, "A6": 0.21526}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:50.424895+00:00"}
------------------------------------------------------------------------
1.356e+01 0.0
1.400e+01 1.651e-21
1.450e+01 9.394e-21
1.500e+01 2.401e-20
1.550e+01 3.904e-20
1.600e+01 7.604e-20
1.650e+01 1.104e-19
1.700e+01 1.218e-19
1.750e+01 1.384e-19
1.800e+01 1.559e-19
1.850e+01 1.706e-19
1.900e+01 1.829e-19
1.950e+01 1.935e-19
2.000e+01 2.03e-19
2.100e+01 2.184e-19
2.200e+01 2.306e-19
2.300e+01 2.405e-19
2.400e+01 2.483e-19
2.500e+01 2.545e-19
2.600e+01 2.594e-19
2.700e+01 2.631e-19
2.800e+01 2.659e-19
2.900e+01 2.679e-19
3.000e+01 2.693e-19
3.500e+01 2.693e-19
4.000e+01 2.625e-19
4.500e+01 2.527e-19
5.000e+01 2.416e-19
6.000e+01 2.193e-19
7.000e+01 1.989e-19
8.000e+01 1.812e-19
9.000e+01 1.66e-19
1.000e+02 1.53e-19
1.250e+02 1.283e-19
1.500e+02 1.115e-19
2.000e+02 9.114e-20
2.500e+02 7.997e-20
3.000e+02 7.28e-20
3.500e+02 6.711e-20
4.000e+02 6.151e-20
4.500e+02 5.522e-20
5.000e+02 4.767e-20