{"qid": "D110218", "reaction": "e- + T2+ 1s-\u03c3g1;v=1 \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=1. 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 16:07:02.606450+00:00"}
------------------------------------------------------------------------
1.150e+01 8.534e-08
1.300e+01 5.1e-08
1.500e+01 0.004464
2.000e+01 1.248
3.000e+01 1.062
4.000e+01 1.085
5.000e+01 1.072
6.000e+01 1.074
7.500e+01 1.044
9.000e+01 1.01
1.000e+02 0.9853
1.150e+02 0.9479
1.300e+02 0.9103
1.500e+02 0.863
1.750e+02 0.8094
2.000e+02 0.759
2.500e+02 0.6734
3.000e+02 0.6055
4.000e+02 0.5045
5.000e+02 0.4331
6.250e+02 0.371
7.500e+02 0.3251
1.000e+03 0.262