{"qid": "D68252", "reaction": "e- + LiH X(1\u03a3+g);v=11 \u2192 LiH A(1\u03a3+g);v=3 + 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": 1.8912, "metadata_version": "M1.0", "time_added": "2022-05-26 11:01:46.906373+00:00"}
------------------------------------------------------------------------
1.900e+00 3.353e-17
2.000e+00 1.113e-16
2.100e+00 1.456e-16
2.200e+00 1.677e-16
2.300e+00 1.832e-16
2.400e+00 1.944e-16
2.500e+00 2.026e-16
2.600e+00 2.087e-16
2.700e+00 2.133e-16
2.800e+00 2.165e-16
2.900e+00 2.188e-16
3.000e+00 2.204e-16
3.100e+00 2.213e-16
3.200e+00 2.218e-16
3.300e+00 2.218e-16
3.400e+00 2.215e-16
3.500e+00 2.21e-16
3.600e+00 2.202e-16
3.700e+00 2.192e-16
3.800e+00 2.181e-16
3.900e+00 2.169e-16
4.000e+00 2.156e-16
4.100e+00 2.142e-16
4.200e+00 2.128e-16
4.300e+00 2.112e-16
4.400e+00 2.097e-16
4.500e+00 2.081e-16
4.600e+00 2.065e-16
4.700e+00 2.049e-16
4.800e+00 2.033e-16
4.900e+00 2.017e-16
5.000e+00 2e-16
5.500e+00 1.92e-16
6.000e+00 1.843e-16
6.500e+00 1.77e-16
7.000e+00 1.703e-16
7.500e+00 1.639e-16
8.000e+00 1.58e-16
8.500e+00 1.525e-16
9.000e+00 1.474e-16
9.500e+00 1.426e-16
1.000e+01 1.382e-16
1.100e+01 1.301e-16
1.200e+01 1.23e-16
1.300e+01 1.167e-16
1.400e+01 1.11e-16
1.500e+01 1.059e-16
2.000e+01 8.657e-17
2.500e+01 7.363e-17
3.000e+01 6.431e-17
3.500e+01 5.725e-17
4.000e+01 5.17e-17
4.500e+01 4.721e-17
5.000e+01 4.349e-17
6.000e+01 3.769e-17
7.000e+01 3.336e-17
8.000e+01 2.998e-17
9.000e+01 2.727e-17
1.000e+02 2.504e-17
1.250e+02 2.088e-17
1.500e+02 1.797e-17
2.000e+02 1.415e-17
2.500e+02 1.174e-17
3.000e+02 1.007e-17
3.500e+02 8.84e-18
4.000e+02 7.892e-18
4.500e+02 7.138e-18
5.000e+02 6.523e-18
6.000e+02 5.579e-18
7.000e+02 4.885e-18
8.000e+02 4.353e-18
9.000e+02 3.93e-18
1.000e+03 3.587e-18