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Electronic structure and resonant inelastic x-ray scattering in Ca3Ru2O7
被引:0
|作者:
Antonov, V. N.
[1
,2
]
Kukusta, D. A.
[1
]
Bekenov, L. V.
[1
]
机构:
[1] NAS Ukraine, GV Kurdyumov Inst Met Phys, UA-03142 Kiev, Ukraine
[2] Max Planck Inst Solid State Res, D-70569 Stuttgart, Germany
来源:
PHYSICAL REVIEW MATERIALS
|
2024年
/
8卷
/
07期
关键词:
SUPERCONDUCTIVITY;
TRANSITION;
BEHAVIOR;
CHARGE;
PHASE;
METAL;
D O I:
10.1103/PhysRevMaterials.8.074401
中图分类号:
T [工业技术];
学科分类号:
08 ;
摘要:
We have investigated the electronic structure of the transition metal oxide Ca3Ru2O7 within density-functional theory using the generalized gradient approximation while considering strong Coulomb correlations in the framework of the fully relativistic spin-polarized Dirac linear muffin-tin orbital band structure method. Ca3Ru2O7 can be classified as a Mott insulator since it was expected to be metallic from band structure calculations. We found that the magnetic ground state of Ca3Ru2O7 possesses an AFM-b magnetic structure with the Ru spin moments ordered antiferromagnetically along the b axis. We have investigated the resonant inelastic x-ray scattering (RIXS) spectra at the Ru and Ca K, L3, and M3 edges as well as at the O K edge. The experimentally measured RIXS spectrum of Ca3Ru2O7 at the Ru L3 edge possesses a sharp feature .2 eV corresponding to transitions within the Ru t2g levels. The excitation located from 2 to 4 eV is due to t2g -> eg transitions. The third wide structure situated at 4.5 - 11 eV appears due to transitions between the Ru 4dO states derived from the tails of oxygen 2p states and eg and t2g states. The RIXS spectra at the Ru L3 and M3 edges are quite similar. However, the corresponding RIXS spectra at the Ca site are quite different from each other due to the significant difference in the widths of core levels. The RIXS spectrum at the O K edge consists of three major inelastic excitations. We found that the first two low energy features .2.5 eV are due to interband transitions between occupied and empty Ot2g states which appear due to the strong hybridization between oxygen 2p and Ru t2g states in close vicinity to the Fermi level. The next major peak between 2.5 and 8 eV reflects interband transitions from occupied O 2p to empty Ot2g states. A wide energy interval between 4 and 11 eV is occupied by rather weak O2p -> Oeg transitions.
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页数:11
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