{"qid": "D110226", "reaction": "e- + T2+ 1s-\u03c3g1;v=9 \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=9. 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 16:07:04.182492+00:00"}
------------------------------------------------------------------------
1.150e+01 4.062e-05
1.300e+01 1.256
1.500e+01 1.324
2.000e+01 1.302
3.000e+01 1.386
4.000e+01 1.443
5.000e+01 1.442
6.000e+01 1.43
7.500e+01 1.386
9.000e+01 1.339
1.000e+02 1.302
1.150e+02 1.247
1.300e+02 1.191
1.500e+02 1.121
1.750e+02 1.042
2.000e+02 0.9723
2.500e+02 0.8554
3.000e+02 0.7648
4.000e+02 0.6326
5.000e+02 0.5423
6.250e+02 0.4617
7.500e+02 0.4032
1.000e+03 0.3239