{"qid": "D68288", "reaction": "e- + LiH X(1\u03a3+g);v=13 \u2192 LiH A(1\u03a3+g);v=10 + e-", "process_types": {"EXE": "Electronic Excitation", "EXV": "Vibrational Excitation"}, "data_type": "cross section", "refs": {"B11": {"doi": "10.1088/1361-6595/ab569e"}}, "comment": "Vibrationally-resolved electron-impact excitation of LiH using Threshold Modified Mott and Massey (TMMM) approximation", "method": "TMMM", "columns": [{"name": "E", "units": "eV"}, {"name": "sigma", "units": "cm2"}], "threshold": 2.0098, "metadata_version": "M1.0", "time_added": "2022-05-26 11:01:47.874378+00:00"} ------------------------------------------------------------------------ 2.025e+00 2.366e-17 2.125e+00 6.15e-17 2.225e+00 7.965e-17 2.325e+00 9.155e-17 2.425e+00 1e-16 2.525e+00 1.062e-16 2.625e+00 1.109e-16 2.725e+00 1.144e-16 2.825e+00 1.171e-16 2.925e+00 1.19e-16 3.025e+00 1.205e-16 3.125e+00 1.215e-16 3.225e+00 1.222e-16 3.325e+00 1.226e-16 3.425e+00 1.227e-16 3.525e+00 1.227e-16 3.625e+00 1.225e-16 3.725e+00 1.222e-16 3.825e+00 1.218e-16 3.925e+00 1.213e-16 4.025e+00 1.208e-16 4.125e+00 1.201e-16 4.225e+00 1.195e-16 4.325e+00 1.188e-16 4.425e+00 1.18e-16 4.525e+00 1.172e-16 4.625e+00 1.164e-16 4.725e+00 1.156e-16 4.825e+00 1.148e-16 4.925e+00 1.14e-16 5.025e+00 1.131e-16 5.500e+00 1.091e-16 6.000e+00 1.05e-16 6.500e+00 1.01e-16 7.000e+00 9.729e-17 7.500e+00 9.378e-17 8.000e+00 9.05e-17 8.500e+00 8.744e-17 9.000e+00 8.457e-17 9.500e+00 8.189e-17 1.000e+01 7.939e-17 1.100e+01 7.483e-17 1.200e+01 7.079e-17 1.300e+01 6.72e-17 1.400e+01 6.398e-17 1.500e+01 6.108e-17 2.000e+01 5.002e-17 2.500e+01 4.26e-17 3.000e+01 3.724e-17 3.500e+01 3.317e-17 4.000e+01 2.997e-17 4.500e+01 2.738e-17 5.000e+01 2.523e-17 6.000e+01 2.188e-17 7.000e+01 1.937e-17 8.000e+01 1.742e-17 9.000e+01 1.584e-17 1.000e+02 1.455e-17 1.250e+02 1.214e-17 1.500e+02 1.045e-17 2.000e+02 8.239e-18 2.500e+02 6.838e-18 3.000e+02 5.866e-18 3.500e+02 5.15e-18 4.000e+02 4.598e-18 4.500e+02 4.16e-18 5.000e+02 3.802e-18 6.000e+02 3.252e-18 7.000e+02 2.848e-18 8.000e+02 2.538e-18 9.000e+02 2.292e-18 1.000e+03 2.092e-18