{"qid": "D110141", "reaction": "e- + H2+ 1s-\u03c3g1;v=4 \u2192 H + H+ + e-", "process_types": {"EDS": "Dissociation"}, "data_type": "cross section", "refs": {"B66": {"doi": "10.1103/physreva.90.022711"}}, "comment": "Convergent close-coupling calculations of electron scattering from H2+ initially in the electronic ground 1sSg, vibrational state v_i=4. Dissociative excitation cross sections (DECS) of the (1sSg, v_i) state, where s refers to orbital angular momentum l = 0, S refers to the symbol sigma (orbital angular momentum projection m = 0) and g refers to the states even parity. The dissociative excitation process: e- + H2+ ---> H(nl) + H+ + e-. Here DECS are calculated as the sum of all electronic excitation cross sections. 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 16:06:47.936047+00:00"} ------------------------------------------------------------------------ 1.000e+01 4.062e-16 1.150e+01 3.933e-16 1.300e+01 3.816e-16 1.500e+01 3.642e-16 2.000e+01 3.521e-16 3.000e+01 2.954e-16 4.000e+01 2.591e-16 5.000e+01 2.334e-16 6.000e+01 2.142e-16 7.500e+01 1.915e-16 9.000e+01 1.741e-16 1.000e+02 1.644e-16 1.150e+02 1.518e-16 1.300e+02 1.41e-16 1.500e+02 1.289e-16 1.750e+02 1.167e-16 2.000e+02 1.066e-16 2.500e+02 9.109e-17 3.000e+02 7.973e-17 4.000e+02 6.412e-17 5.000e+02 5.389e-17 6.250e+02 4.513e-17 7.500e+02 3.894e-17 1.000e+03 3.075e-17