{"qid": "D110271", "reaction": "e- + T2+ 1s-\u03c3g1;v=17 \u2192 T + T+ + 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 T2+ initially in the electronic ground 1sSg, vibrational state v_i=17. 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- + T2+ ---> T(nl) + T+ + 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 16:07:12.555036+00:00"} ------------------------------------------------------------------------ 1.000e+01 1.503e-15 1.150e+01 1.416e-15 1.300e+01 1.352e-15 1.500e+01 1.249e-15 2.000e+01 1.072e-15 3.000e+01 8.427e-16 4.000e+01 7.078e-16 5.000e+01 6.153e-16 6.000e+01 5.487e-16 7.500e+01 4.732e-16 9.000e+01 4.181e-16 1.000e+02 3.886e-16 1.150e+02 3.52e-16 1.300e+02 3.219e-16 1.500e+02 2.895e-16 1.750e+02 2.576e-16 2.000e+02 2.324e-16 2.500e+02 1.949e-16 3.000e+02 1.683e-16 4.000e+02 1.329e-16 5.000e+02 1.103e-16 6.250e+02 9.13e-17 7.500e+02 7.806e-17 1.000e+03 6.069e-17