{"qid": "D2309", "reaction": "e- + D2 X(1\u03a3+g);v=9 \u2192 D2 D(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": 13.8264, "fit": {"coeffs": {"A1": 0.40195, "A2": 0.4103, "A3": -2.4354, "A4": 5.4971, "A5": -5.5336, "A6": 2.0683}, "func": "singlet_singlet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:40:49.983602+00:00"}
------------------------------------------------------------------------
1.383e+01 0.0
1.400e+01 2.158e-22
1.450e+01 3.68e-21
1.500e+01 1.487e-20
1.550e+01 3.08e-20
1.600e+01 5.224e-20
1.650e+01 8.608e-20
1.700e+01 1.183e-19
1.750e+01 1.516e-19
1.800e+01 1.903e-19
1.850e+01 2.293e-19
1.900e+01 2.682e-19
1.950e+01 3.066e-19
2.000e+01 3.443e-19
2.100e+01 4.172e-19
2.200e+01 4.866e-19
2.300e+01 5.524e-19
2.400e+01 6.147e-19
2.500e+01 6.737e-19
2.600e+01 7.294e-19
2.700e+01 7.821e-19
2.800e+01 8.321e-19
2.900e+01 8.793e-19
3.000e+01 9.241e-19
3.500e+01 1.115e-18
4.000e+01 1.26e-18
4.500e+01 1.37e-18
5.000e+01 1.454e-18
6.000e+01 1.562e-18
7.000e+01 1.617e-18
8.000e+01 1.637e-18
9.000e+01 1.635e-18
1.000e+02 1.618e-18
1.250e+02 1.542e-18
1.500e+02 1.448e-18
2.000e+02 1.265e-18
2.500e+02 1.112e-18
3.000e+02 9.906e-19
3.500e+02 8.936e-19
4.000e+02 8.15e-19
4.500e+02 7.496e-19
5.000e+02 6.934e-19