{"qid": "D110251", "reaction": "e- + T2+ 1s-\u03c3g1;v=15 \u2192 T2+ 2p-\u03c3u1 + e-", "process_types": {"EXE": "Electronic Excitation"}, "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=15. Integrated cross sections for the transition (1sSg, v_i) ---> 2pSu, 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) 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).", "method": "theory", "columns": [{"name": "E", "units": "eV"}, {"name": "sigma", "units": "cm2"}], "from_aladdin": true, "metadata_version": "M1.0", "time_added": "2023-02-09 16:07:08.762280+00:00"}
------------------------------------------------------------------------
1.000e+01 1.144e-15
1.150e+01 1.045e-15
1.300e+01 9.615e-16
1.500e+01 8.643e-16
2.000e+01 7.31e-16
3.000e+01 5.649e-16
4.000e+01 4.724e-16
5.000e+01 4.075e-16
6.000e+01 3.595e-16
7.500e+01 3.075e-16
9.000e+01 2.694e-16
1.000e+02 2.492e-16
1.150e+02 2.244e-16
1.300e+02 2.043e-16
1.500e+02 1.829e-16
1.750e+02 1.62e-16
2.000e+02 1.456e-16
2.500e+02 1.215e-16
3.000e+02 1.046e-16
4.000e+02 8.219e-17
5.000e+02 6.798e-17
6.250e+02 5.612e-17
7.500e+02 4.791e-17
1.000e+03 3.721e-17