{"qid": "D9619", "reaction": "e- + H2+ 1s-\u03c3g1;v=7 \u2192 H2+ 2p-\u03c0u1 + e-", "process_types": {"EXE": "Electronic Excitation"}, "data_type": "cross section", "refs": {"B17": {"doi": "10.1103/physreva.90.022711"}}, "json_comment": {"comment": "Convergent close-coupling calculations of electron scattering from H2+ 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)."}, "json_data": {"method": "theory", "columns": [{"name": "E", "units": "eV"}, {"name": "sigma", "units": "cm2"}]}}
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1.150e+01 3.332e-18
1.300e+01 4.939e-17
1.500e+01 4.016e-17
2.000e+01 3.972e-17
3.000e+01 4.235e-17
4.000e+01 4.436e-17
5.000e+01 4.441e-17
6.000e+01 4.403e-17
7.500e+01 4.279e-17
9.000e+01 4.124e-17
1.000e+02 4.002e-17
1.150e+02 3.823e-17
1.300e+02 3.646e-17
1.500e+02 3.424e-17
1.750e+02 3.174e-17
2.000e+02 2.956e-17
2.500e+02 2.593e-17
3.000e+02 2.314e-17
4.000e+02 1.911e-17
5.000e+02 1.635e-17
6.250e+02 1.39e-17
7.500e+02 1.213e-17
1.000e+03 9.734e-18