{"qid": "D110308", "reaction": "e- + HD+ 1s-\u03c3g1;v=6 \u2192 HD+ 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 HD+ initially in the electronic ground 1sSg, vibrational state v_i=6. 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 16:07:19.574185+00:00"} ------------------------------------------------------------------------ 1.000e+01 5.318e-16 1.150e+01 5.046e-16 1.300e+01 4.648e-16 1.500e+01 4.183e-16 2.000e+01 3.54e-16 3.000e+01 2.763e-16 4.000e+01 2.37e-16 5.000e+01 2.086e-16 6.000e+01 1.866e-16 7.500e+01 1.625e-16 9.000e+01 1.441e-16 1.000e+02 1.343e-16 1.150e+02 1.221e-16 1.300e+02 1.121e-16 1.500e+02 1.012e-16 1.750e+02 9.035e-17 2.000e+02 8.173e-17 2.500e+02 6.886e-17 3.000e+02 5.968e-17 4.000e+02 4.738e-17 5.000e+02 3.947e-17 6.250e+02 3.28e-17 7.500e+02 2.815e-17 1.000e+03 2.206e-17