{"qid": "D2256", "reaction": "e- + D2 X(1\u03a3+g);v=20 \u2192 D2 C(1\u03a0u) + 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": 10.2218, "fit": {"coeffs": {"A1": 0.69264, "A2": 0.50215, "A3": -4.4797, "A4": 11.572, "A5": -12.357, "A6": 4.8385}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:35.499523+00:00"}
------------------------------------------------------------------------
1.022e+01 0.0
1.050e+01 1.595e-20
1.150e+01 1.451e-19
1.200e+01 2.39e-19
1.250e+01 3.526e-19
1.300e+01 4.632e-19
1.350e+01 5.625e-19
1.400e+01 6.563e-19
1.450e+01 7.566e-19
1.500e+01 8.531e-19
1.550e+01 9.466e-19
1.600e+01 1.036e-18
1.650e+01 1.125e-18
1.700e+01 1.21e-18
1.750e+01 1.293e-18
1.800e+01 1.372e-18
1.850e+01 1.449e-18
1.900e+01 1.522e-18
1.950e+01 1.593e-18
2.000e+01 1.661e-18
2.100e+01 1.789e-18
2.200e+01 1.907e-18
2.300e+01 2.017e-18
2.400e+01 2.12e-18
2.500e+01 2.215e-18
2.600e+01 2.304e-18
2.700e+01 2.387e-18
2.800e+01 2.465e-18
2.900e+01 2.537e-18
3.000e+01 2.604e-18
3.500e+01 2.881e-18
4.000e+01 3.078e-18
4.500e+01 3.216e-18
5.000e+01 3.309e-18
6.000e+01 3.402e-18
7.000e+01 3.416e-18
8.000e+01 3.381e-18
9.000e+01 3.317e-18
1.000e+02 3.236e-18
1.250e+02 3.001e-18
1.500e+02 2.764e-18
2.000e+02 2.353e-18
2.500e+02 2.042e-18
3.000e+02 1.809e-18
3.500e+02 1.63e-18
4.000e+02 1.488e-18
4.500e+02 1.37e-18
5.000e+02 1.267e-18