{"qid": "D3042", "reaction": "e- + H2 X(1\u03a3+g);v=8 \u2192 H2 B'(1\u03a3+u) + 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": 11.3542, "fit": {"coeffs": {"A1": 0.65684, "A2": 0.56963, "A3": -2.597, "A4": 5.1541, "A5": -3.9131, "A6": 0.9646}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:13.200695+00:00"} ------------------------------------------------------------------------ 1.135e+01 0.0 1.150e+01 4.085e-20 1.200e+01 2.319e-19 1.250e+01 5.017e-19 1.300e+01 7.82e-19 1.350e+01 1.003e-18 1.400e+01 1.225e-18 1.450e+01 1.383e-18 1.500e+01 1.534e-18 1.550e+01 1.685e-18 1.600e+01 1.819e-18 1.650e+01 1.946e-18 1.700e+01 2.063e-18 1.750e+01 2.172e-18 1.800e+01 2.275e-18 1.850e+01 2.373e-18 1.900e+01 2.466e-18 1.950e+01 2.553e-18 2.000e+01 2.636e-18 2.100e+01 2.789e-18 2.200e+01 2.927e-18 2.300e+01 3.051e-18 2.400e+01 3.164e-18 2.500e+01 3.265e-18 2.600e+01 3.358e-18 2.700e+01 3.441e-18 2.800e+01 3.517e-18 2.900e+01 3.586e-18 3.000e+01 3.648e-18 3.500e+01 3.88e-18 4.000e+01 4.015e-18 4.500e+01 4.085e-18 5.000e+01 4.111e-18 6.000e+01 4.082e-18 7.000e+01 3.991e-18 8.000e+01 3.872e-18 9.000e+01 3.741e-18 1.000e+02 3.607e-18 1.250e+02 3.286e-18 1.500e+02 3e-18 2.000e+02 2.539e-18 2.500e+02 2.194e-18 3.000e+02 1.929e-18 3.500e+02 1.721e-18 4.000e+02 1.553e-18 4.500e+02 1.414e-18 5.000e+02 1.299e-18