{"qid": "D110232", "reaction": "e- + T2+ 1s-\u03c3g1;v=15 \u2192 T2+ 2p-\u03c0u1 + 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) ---> 2pPu, 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), P refers to the symbol pi (orbital angular momentum projection |m| = 1), 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 16:07:05.341800+00:00"}
------------------------------------------------------------------------
1.150e+01 1.282
1.300e+01 1.866
1.500e+01 1.576
2.000e+01 1.484
3.000e+01 1.59
4.000e+01 1.677
5.000e+01 1.68
6.000e+01 1.668
7.500e+01 1.622
9.000e+01 1.56
1.000e+02 1.512
1.150e+02 1.443
1.300e+02 1.374
1.500e+02 1.288
1.750e+02 1.192
2.000e+02 1.109
2.500e+02 0.9714
3.000e+02 0.8654
4.000e+02 0.7141
5.000e+02 0.6103
6.250e+02 0.5182
7.500e+02 0.452
1.000e+03 0.3626