{"qid": "D110167", "reaction": "e- + D2+ 1s-\u03c3g1;v=9 \u2192 D2+ 2p-\u03c0u1 + e-", "process_types": {"EXE": "Electronic Excitation"}, "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=9. Integrated cross sections for the transition (1sSg, v_i) ---> 2pPu, where s and p refers to orbital angular momentum l = 0 and l = 1, respectively, S refers to the symbol sigma (orbital angular momentum projection m = 0), P refers to the symbol pi (orbital angular momentum projection |m| = 1), and g and u refers to states even or odd parity, respectively. 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 16:06:52.995042+00:00"}
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1.150e+01 3.369e-19
1.300e+01 4.647e-17
1.500e+01 3.819e-17
2.000e+01 3.849e-17
3.000e+01 4.104e-17
4.000e+01 4.287e-17
5.000e+01 4.29e-17
6.000e+01 4.252e-17
7.500e+01 4.128e-17
9.000e+01 3.982e-17
1.000e+02 3.868e-17
1.150e+02 3.698e-17
1.300e+02 3.529e-17
1.500e+02 3.317e-17
1.750e+02 3.078e-17
2.000e+02 2.869e-17
2.500e+02 2.519e-17
3.000e+02 2.249e-17
4.000e+02 1.859e-17
5.000e+02 1.592e-17
6.250e+02 1.354e-17
7.500e+02 1.182e-17
1.000e+03 9.487e-18