{"qid": "D110314", "reaction": "e- + HD+ 1s-\u03c3g1;v=0 \u2192 H + D+ + 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 HD+ initially in the electronic ground 1sSg, vibrational state v_i=0. 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- + AB+ ---> A(nl) + B+ + 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 16:07:20.638619+00:00"} ------------------------------------------------------------------------ 1.000e+01 4.627e-17 1.150e+01 8.681e-17 1.300e+01 1.208e-16 1.500e+01 1.261e-16 2.000e+01 1.57e-16 3.000e+01 1.473e-16 4.000e+01 1.335e-16 5.000e+01 1.213e-16 6.000e+01 1.138e-16 7.500e+01 1.047e-16 9.000e+01 9.72e-17 1.000e+02 9.29e-17 1.150e+02 8.723e-17 1.300e+02 8.207e-17 1.500e+02 7.618e-17 1.750e+02 6.994e-17 2.000e+02 6.461e-17 2.500e+02 5.611e-17 3.000e+02 4.968e-17 4.000e+02 4.06e-17 5.000e+02 3.443e-17 6.250e+02 2.909e-17 7.500e+02 2.526e-17 1.000e+03 2.01e-17