{"qid": "D2180", "reaction": "e- + D2 X(1\u03a3+g);v=11 \u2192 D2 B(1\u03a3+u) + e-", "process_types": {"EDE": "Dissociative Excitation"}, "data_type": "cross section", "refs": {"B9": {"doi": "10.1016/j.adt.2020.101403"}}, "comment": "MCCC calculations of vibrationally-resolved electron-impact dissociative excitation of D2, 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": 11.4661, "fit": {"coeffs": {"A1": 0.90197, "A2": 0.78134, "A3": -6.0795, "A4": 15.122, "A5": -15.796, "A6": 6.0378}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:14.699411+00:00"} ------------------------------------------------------------------------ 1.147e+01 0.0 1.150e+01 1.023e-21 1.200e+01 4.175e-20 1.250e+01 1.375e-19 1.300e+01 2.979e-19 1.350e+01 4.522e-19 1.400e+01 6.372e-19 1.450e+01 8.166e-19 1.500e+01 1.006e-18 1.550e+01 1.181e-18 1.600e+01 1.369e-18 1.650e+01 1.555e-18 1.700e+01 1.736e-18 1.750e+01 1.911e-18 1.800e+01 2.079e-18 1.850e+01 2.24e-18 1.900e+01 2.395e-18 1.950e+01 2.544e-18 2.000e+01 2.687e-18 2.100e+01 2.956e-18 2.200e+01 3.205e-18 2.300e+01 3.435e-18 2.400e+01 3.647e-18 2.500e+01 3.843e-18 2.600e+01 4.024e-18 2.700e+01 4.192e-18 2.800e+01 4.347e-18 2.900e+01 4.492e-18 3.000e+01 4.625e-18 3.500e+01 5.162e-18 4.000e+01 5.53e-18 4.500e+01 5.779e-18 5.000e+01 5.941e-18 6.000e+01 6.093e-18 7.000e+01 6.101e-18 8.000e+01 6.028e-18 9.000e+01 5.909e-18 1.000e+02 5.765e-18 1.250e+02 5.367e-18 1.500e+02 4.972e-18 2.000e+02 4.285e-18 2.500e+02 3.743e-18 3.000e+02 3.316e-18 3.500e+02 2.978e-18 4.000e+02 2.705e-18 4.500e+02 2.484e-18 5.000e+02 2.304e-18