{"qid": "D3129", "reaction": "e- + H2 X(1\u03a3+g);v=5 \u2192 H2 EF(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": 12.388, "fit": {"coeffs": {"A1": -9.9201e-05, "A2": 0.33063, "A3": -0.37448, "A4": -2.3337, "A5": 7.6042, "A6": -5.4965}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:37.288824+00:00"}
------------------------------------------------------------------------
1.239e+01 0.0
1.250e+01 9.636e-22
1.300e+01 3.272e-20
1.350e+01 8.793e-20
1.400e+01 2.652e-19
1.450e+01 3.342e-19
1.500e+01 4.184e-19
1.550e+01 6.111e-19
1.600e+01 8.2e-19
1.650e+01 1.135e-18
1.700e+01 1.384e-18
1.750e+01 1.411e-18
1.800e+01 1.412e-18
1.850e+01 1.394e-18
1.900e+01 1.361e-18
1.950e+01 1.302e-18
2.000e+01 1.254e-18
2.100e+01 1.23e-18
2.200e+01 1.211e-18
2.300e+01 1.188e-18
2.400e+01 1.163e-18
2.500e+01 1.141e-18
2.600e+01 1.119e-18
2.700e+01 1.097e-18
2.800e+01 1.078e-18
2.900e+01 1.063e-18
3.000e+01 1.054e-18
3.500e+01 1.046e-18
4.000e+01 1.045e-18
4.500e+01 1.026e-18
5.000e+01 9.955e-19
6.000e+01 9.48e-19
7.000e+01 8.987e-19
8.000e+01 8.544e-19
9.000e+01 8.163e-19
1.000e+02 7.824e-19
1.250e+02 7.085e-19
1.500e+02 6.429e-19
2.000e+02 5.249e-19
2.500e+02 4.146e-19
3.000e+02 3.31e-19
3.500e+02 2.878e-19
4.000e+02 2.591e-19
4.500e+02 2.308e-19
5.000e+02 2.13e-19