{"qid": "D9614", "reaction": "e- + H2+ 1s-\u03c3g1;v=2 \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=2. 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"}]}}
------------------------------------------------------------------------
1.150e+01 3.362e-22
1.300e+01 4.172e-20
1.500e+01 1.691e-17
2.000e+01 3.059e-17
3.000e+01 3.312e-17
4.000e+01 3.407e-17
5.000e+01 3.384e-17
6.000e+01 3.378e-17
7.500e+01 3.267e-17
9.000e+01 3.157e-17
1.000e+02 3.076e-17
1.150e+02 2.957e-17
1.300e+02 2.835e-17
1.500e+02 2.68e-17
1.750e+02 2.504e-17
2.000e+02 2.343e-17
2.500e+02 2.072e-17
3.000e+02 1.859e-17
4.000e+02 1.544e-17
5.000e+02 1.326e-17
6.250e+02 1.132e-17
7.500e+02 9.909e-18
1.000e+03 7.974e-18