{"qid": "D110200", "reaction": "e- + D2+ 1s-\u03c3g1;v=12 \u2192 D + D+ + e-", "process_types": {"EDS": "Dissociation"}, "data_type": "cross section", "refs": {"B66": {"doi": "10.1103/physreva.90.022711"}}, "comment": "Convergent close-coupling calculations of electron scattering from D2+ initially in the electronic ground 1sSg, vibrational state v_i=12. Dissociative excitation cross sections (DECS) of the (1sSg, v_i) state, where s refers to orbital angular momentum l = 0, S refers to the symbol sigma (orbital angular momentum projection m = 0) and g refers to the states even parity. The dissociative excitation process: e- + D2+ ---> D(nl)  + D+ + e-. Here DECS are calculated as the sum of all electronic excitation cross sections. Cross sections are calculated in the adiabatic-nuclei approximation where the cross section have been summed analytically over all final rotational and vibrational states. These cross sections were calculated with a 351-state CCC calculation. To reference and for details see M. C. Zammit, D. V. Fursa, and I. Bray, Phys. Rev. A 90, 022711 (2014).", "method": "theory", "columns": [{"name": "E", "units": "eV"}, {"name": "sigma", "units": "cm2"}], "from_aladdin": true, "metadata_version": "M1.0", "time_added": "2023-02-09 16:06:59.073240+00:00"}
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1.000e+01 1.115e-15
1.150e+01 1.048e-15
1.300e+01 1.007e-15
1.500e+01 9.502e-16
2.000e+01 8.138e-16
3.000e+01 6.519e-16
4.000e+01 5.536e-16
5.000e+01 4.853e-16
6.000e+01 4.352e-16
7.500e+01 3.79e-16
9.000e+01 3.369e-16
1.000e+02 3.142e-16
1.150e+02 2.857e-16
1.300e+02 2.622e-16
1.500e+02 2.366e-16
1.750e+02 2.113e-16
2.000e+02 1.911e-16
2.500e+02 1.609e-16
3.000e+02 1.394e-16
4.000e+02 1.106e-16
5.000e+02 9.204e-17
6.250e+02 7.641e-17
7.500e+02 6.552e-17
1.000e+03 5.122e-17