{"qid": "D3001", "reaction": "e- + H2 X(1\u03a3+g);v=11 \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": 10.6035, "fit": {"coeffs": {"A1": 0.92215, "A2": 0.41802, "A3": -4.4436, "A4": 11.557, "A5": -11.774, "A6": 4.2866}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:01.772633+00:00"} ------------------------------------------------------------------------ 1.060e+01 0.0 1.150e+01 1.277e-19 1.200e+01 2.883e-19 1.250e+01 4.988e-19 1.300e+01 7.034e-19 1.350e+01 9.328e-19 1.400e+01 1.138e-18 1.450e+01 1.324e-18 1.500e+01 1.51e-18 1.550e+01 1.679e-18 1.600e+01 1.851e-18 1.650e+01 2.021e-18 1.700e+01 2.184e-18 1.750e+01 2.34e-18 1.800e+01 2.489e-18 1.850e+01 2.631e-18 1.900e+01 2.767e-18 1.950e+01 2.897e-18 2.000e+01 3.02e-18 2.100e+01 3.252e-18 2.200e+01 3.464e-18 2.300e+01 3.658e-18 2.400e+01 3.836e-18 2.500e+01 4e-18 2.600e+01 4.15e-18 2.700e+01 4.288e-18 2.800e+01 4.416e-18 2.900e+01 4.533e-18 3.000e+01 4.64e-18 3.500e+01 5.065e-18 4.000e+01 5.343e-18 4.500e+01 5.52e-18 5.000e+01 5.626e-18 6.000e+01 5.695e-18 7.000e+01 5.652e-18 8.000e+01 5.548e-18 9.000e+01 5.411e-18 1.000e+02 5.258e-18 1.250e+02 4.86e-18 1.500e+02 4.484e-18 2.000e+02 3.847e-18 2.500e+02 3.354e-18 3.000e+02 2.97e-18 3.500e+02 2.667e-18 4.000e+02 2.422e-18 4.500e+02 2.223e-18 5.000e+02 2.058e-18