{"qid": "D110297", "reaction": "e- + HD+ 1s-\u03c3g1;v=7 \u2192 HD+ 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 HD+ 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 16:07:17.550051+00:00"}
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1.150e+01 2.002e-19
1.300e+01 4.931e-17
1.500e+01 3.938e-17
2.000e+01 3.797e-17
3.000e+01 4.063e-17
4.000e+01 4.243e-17
5.000e+01 4.243e-17
6.000e+01 4.207e-17
7.500e+01 4.083e-17
9.000e+01 3.941e-17
1.000e+02 3.828e-17
1.150e+02 3.662e-17
1.300e+02 3.495e-17
1.500e+02 3.286e-17
1.750e+02 3.049e-17
2.000e+02 2.843e-17
2.500e+02 2.497e-17
3.000e+02 2.23e-17
4.000e+02 1.844e-17
5.000e+02 1.579e-17
6.250e+02 1.343e-17
7.500e+02 1.172e-17
1.000e+03 9.413e-18