{"qid": "D110143", "reaction": "e- + H2+ 1s-\u03c3g1;v=6 \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=6. 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 16:06:48.321598+00:00"} ------------------------------------------------------------------------ 1.000e+01 6.515e-16 1.150e+01 6.222e-16 1.300e+01 6.093e-16 1.500e+01 5.661e-16 2.000e+01 5.097e-16 3.000e+01 4.193e-16 4.000e+01 3.633e-16 5.000e+01 3.241e-16 6.000e+01 2.941e-16 7.500e+01 2.597e-16 9.000e+01 2.336e-16 1.000e+02 2.193e-16 1.150e+02 2.011e-16 1.300e+02 1.857e-16 1.500e+02 1.688e-16 1.750e+02 1.517e-16 2.000e+02 1.379e-16 2.500e+02 1.17e-16 3.000e+02 1.019e-16 4.000e+02 8.147e-17 5.000e+02 6.817e-17 6.250e+02 5.686e-17 7.500e+02 4.893e-17 1.000e+03 3.848e-17