{"qid": "D3048", "reaction": "e- + H2 X(1\u03a3+g);v=12 \u2192 H2 C(1\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": 10.4282, "fit": {"coeffs": {"A1": 1.0614, "A2": 0.93867, "A3": -9.5529, "A4": 25.371, "A5": -27.551, "A6": 10.913}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:14.828703+00:00"} ------------------------------------------------------------------------ 1.043e+01 0.0 1.050e+01 1.303e-21 1.150e+01 1.398e-19 1.200e+01 2.752e-19 1.250e+01 4.661e-19 1.300e+01 6.822e-19 1.350e+01 9.171e-19 1.400e+01 1.148e-18 1.450e+01 1.361e-18 1.500e+01 1.565e-18 1.550e+01 1.766e-18 1.600e+01 1.967e-18 1.650e+01 2.17e-18 1.700e+01 2.368e-18 1.750e+01 2.559e-18 1.800e+01 2.742e-18 1.850e+01 2.918e-18 1.900e+01 3.088e-18 1.950e+01 3.251e-18 2.000e+01 3.407e-18 2.100e+01 3.703e-18 2.200e+01 3.978e-18 2.300e+01 4.233e-18 2.400e+01 4.471e-18 2.500e+01 4.692e-18 2.600e+01 4.898e-18 2.700e+01 5.09e-18 2.800e+01 5.27e-18 2.900e+01 5.438e-18 3.000e+01 5.595e-18 3.500e+01 6.241e-18 4.000e+01 6.704e-18 4.500e+01 7.032e-18 5.000e+01 7.258e-18 6.000e+01 7.501e-18 7.000e+01 7.558e-18 8.000e+01 7.503e-18 9.000e+01 7.38e-18 1.000e+02 7.215e-18 1.250e+02 6.726e-18 1.500e+02 6.222e-18 2.000e+02 5.335e-18 2.500e+02 4.645e-18 3.000e+02 4.12e-18 3.500e+02 3.713e-18 4.000e+02 3.389e-18 4.500e+02 3.119e-18 5.000e+02 2.884e-18