{"qid": "D110178", "reaction": "e- + D2+ 1s-\u03c3g1;v=5 \u2192 D2+ 2p-\u03c3u1 + 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=5. Integrated cross sections for the transition (1sSg, v_i) ---> 2pSu, 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) 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 16:06:55.021700+00:00"} ------------------------------------------------------------------------ 1.000e+01 3.488e-16 1.150e+01 3.415e-16 1.300e+01 3.267e-16 1.500e+01 2.809e-16 2.000e+01 2.463e-16 3.000e+01 1.925e-16 4.000e+01 1.669e-16 5.000e+01 1.48e-16 6.000e+01 1.333e-16 7.500e+01 1.174e-16 9.000e+01 1.05e-16 1.000e+02 9.832e-17 1.150e+02 8.986e-17 1.300e+02 8.279e-17 1.500e+02 7.509e-17 1.750e+02 6.748e-17 2.000e+02 6.13e-17 2.500e+02 5.196e-17 3.000e+02 4.521e-17 4.000e+02 3.61e-17 5.000e+02 3.019e-17 6.250e+02 2.518e-17 7.500e+02 2.167e-17 1.000e+03 1.704e-17