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Figure 5
(a, b) 2p3d RIXS simulations of the 1A1g(Oh) ground state as a function of the sample rotation angle α with respect to (a) H-polarization and (b) V-polarization. Small broadening (20 meV) is used in the simulations. (c, d) 2p3d RIXS transition cross-section of the 3T1g excited state as a function of the rotation angle α with respect to (c) H-polarization and (d) V-polarization. Presented here are only the states with a total moment equal to two (j = 2). The scattering angle is now replaced by 90°.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 27| Part 4| July 2020| Pages 979-987
https://doi.org/10.1107/S1600577520005123
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