{"qid": "D3070", "reaction": "e- + H2 X(1\u03a3+g);v=6 \u2192 H2 c(3\u03a0u) + 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": 12.0144, "fit": {"coeffs": {"A1": -1.3848e-05, "A2": 0.13096, "A3": -0.21227, "A4": 3.3578, "A5": -3.3809}, "func": "singlet_triplet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:20.872736+00:00"}
------------------------------------------------------------------------
1.201e+01 0.0
1.250e+01 7.473e-20
1.300e+01 2.349e-19
1.350e+01 4.229e-19
1.400e+01 7.724e-19
1.450e+01 9.19e-19
1.500e+01 1.284e-18
1.550e+01 1.641e-18
1.600e+01 1.87e-18
1.650e+01 1.992e-18
1.700e+01 2.055e-18
1.750e+01 2.08e-18
1.800e+01 2.079e-18
1.850e+01 2.06e-18
1.900e+01 2.027e-18
1.950e+01 1.986e-18
2.000e+01 1.938e-18
2.100e+01 1.831e-18
2.200e+01 1.717e-18
2.300e+01 1.604e-18
2.400e+01 1.495e-18
2.500e+01 1.392e-18
2.600e+01 1.295e-18
2.700e+01 1.205e-18
2.800e+01 1.121e-18
2.900e+01 1.044e-18
3.000e+01 9.737e-19
3.500e+01 6.966e-19
4.000e+01 5.126e-19
4.500e+01 3.874e-19
5.000e+01 2.997e-19
6.000e+01 1.901e-19
7.000e+01 1.282e-19
8.000e+01 9.07e-20
9.000e+01 6.66e-20
1.000e+02 5.04e-20
1.250e+02 2.775e-20
1.500e+02 1.695e-20