{"qid": "D110184", "reaction": "e- + D2+ 1s-\u03c3g1;v=11 \u2192 D2+ 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 D2+ initially in the electronic ground 1sSg, vibrational state v_i=11. 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 16:06:56.043415+00:00"}
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1.000e+01 9.478e-16
1.150e+01 8.731e-16
1.300e+01 7.997e-16
1.500e+01 7.091e-16
2.000e+01 6.089e-16
3.000e+01 4.712e-16
4.000e+01 3.97e-16
5.000e+01 3.442e-16
6.000e+01 3.044e-16
7.500e+01 2.615e-16
9.000e+01 2.298e-16
1.000e+02 2.13e-16
1.150e+02 1.922e-16
1.300e+02 1.753e-16
1.500e+02 1.572e-16
1.750e+02 1.395e-16
2.000e+02 1.256e-16
2.500e+02 1.05e-16
3.000e+02 9.053e-17
4.000e+02 7.133e-17
5.000e+02 5.909e-17
6.250e+02 4.886e-17
7.500e+02 4.178e-17
1.000e+03 3.254e-17