{"qid": "D110165", "reaction": "e- + D2+ 1s-\u03c3g1;v=7 \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=7. 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 16:06:52.605221+00:00"}
------------------------------------------------------------------------
1.150e+01 1.523e-21
1.300e+01 2.714e-17
1.500e+01 3.481e-17
2.000e+01 3.609e-17
3.000e+01 3.849e-17
4.000e+01 4.002e-17
5.000e+01 4e-17
6.000e+01 3.968e-17
7.500e+01 3.843e-17
9.000e+01 3.712e-17
1.000e+02 3.611e-17
1.150e+02 3.46e-17
1.300e+02 3.306e-17
1.500e+02 3.112e-17
1.750e+02 2.893e-17
2.000e+02 2.7e-17
2.500e+02 2.376e-17
3.000e+02 2.125e-17
4.000e+02 1.758e-17
5.000e+02 1.507e-17
6.250e+02 1.283e-17
7.500e+02 1.121e-17
1.000e+03 9.006e-18