TY - JOUR
T1 - Charge transfer satellites and multiplet splitting in X-ray photoemission spectra of late transition metal halides
AU - Okada, K.
AU - Kotani, A.
AU - Thole, B. T.
N1 - Funding Information:
We would like to thank Professor G.A. Sawatzky for useful discussions. This work was partially supported by a Grant-in-Aid for Scientific Research from the Ministry of Education, Science and Culture of Japan, and by an International Joint Research Project from JSPS.
PY - 1992/6/1
Y1 - 1992/6/1
N2 - Core-level X-ray photoemission spectra (XPS) are calculated for Ni and Co dihalides with an MX6 cluster model (M = Ni, Co; X = F, Cl, Br), where intra-atomic multiplet coupling as well as covalency mixing is taken into account. The effects of the intra-atomic configuration interaction between (3s)1(3p)6(3d)n and (3s)2(3p)4(3d)n+1, which is known to be important in the 3s XPS, are treated phenomenologically. The overall spectral shape of the Ni (Co) 2p XPS can be explained by a charge transfer mechanism, and the difference in the line shape between the Ni (Co) 2p 3 2 and 2p 1 2 XPS spectra is shown to originate from the multiplet splitting of their charge transfer satellites. However, the Ni (Co) 3s XPS are so complex that it is difficult to discriminate between exchange split pairs and their charge transfer satellites. As for Co dihalides, the spectral splitting of the 3s XPS mostly represents the 3s-3d exchange splitting of the (3s)1(3d)8 configuration. However, in Ni dihalides the first satellite peak is mainly due to charge transfer.
AB - Core-level X-ray photoemission spectra (XPS) are calculated for Ni and Co dihalides with an MX6 cluster model (M = Ni, Co; X = F, Cl, Br), where intra-atomic multiplet coupling as well as covalency mixing is taken into account. The effects of the intra-atomic configuration interaction between (3s)1(3p)6(3d)n and (3s)2(3p)4(3d)n+1, which is known to be important in the 3s XPS, are treated phenomenologically. The overall spectral shape of the Ni (Co) 2p XPS can be explained by a charge transfer mechanism, and the difference in the line shape between the Ni (Co) 2p 3 2 and 2p 1 2 XPS spectra is shown to originate from the multiplet splitting of their charge transfer satellites. However, the Ni (Co) 3s XPS are so complex that it is difficult to discriminate between exchange split pairs and their charge transfer satellites. As for Co dihalides, the spectral splitting of the 3s XPS mostly represents the 3s-3d exchange splitting of the (3s)1(3d)8 configuration. However, in Ni dihalides the first satellite peak is mainly due to charge transfer.
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U2 - 10.1016/0368-2048(92)85018-3
DO - 10.1016/0368-2048(92)85018-3
M3 - Article
AN - SCOPUS:0000818710
SN - 0368-2048
VL - 58
SP - 325
EP - 343
JO - Journal of Electron Spectroscopy and Related Phenomena
JF - Journal of Electron Spectroscopy and Related Phenomena
IS - 4
ER -