1985
DOI: 10.1103/physrevb.32.4292
|View full text |Cite
|
Sign up to set email alerts
|

X-ray-absorption near-edge structure of3dtransition elements in tetrahedral coordination: The effect of bond-length variation

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

12
98
0

Year Published

1987
1987
2023
2023

Publication Types

Select...
9
1

Relationship

0
10

Authors

Journals

citations
Cited by 162 publications
(110 citation statements)
references
References 7 publications
12
98
0
Order By: Relevance
“…This phenomenon reflects the relation DE / 1/d 2 for a XANES resonance, in where DE denotes an energy difference of absorption feature relative to the ionization threshold and d represents the corresponding interatomic distance. 21 The observed features in the Ti K-edge near-edge spectra of FeTiO 3 at greater energy for E// ab and at smaller energy for E//c are then related to the smaller inter-atomic distance in the ab plane and the larger one in the c direction, respectively. Figure 4(a) shows the polarization-dependent Fe K-edge XANES spectra of FeTiO 3 .…”
mentioning
confidence: 93%
“…This phenomenon reflects the relation DE / 1/d 2 for a XANES resonance, in where DE denotes an energy difference of absorption feature relative to the ionization threshold and d represents the corresponding interatomic distance. 21 The observed features in the Ti K-edge near-edge spectra of FeTiO 3 at greater energy for E// ab and at smaller energy for E//c are then related to the smaller inter-atomic distance in the ab plane and the larger one in the c direction, respectively. Figure 4(a) shows the polarization-dependent Fe K-edge XANES spectra of FeTiO 3 .…”
mentioning
confidence: 93%
“…Reduction in peak intensity and an increased "white-line" at ∼5.488 keV compared to V 2 O 5 suggest a subtle change in the local electronic environment that may be due to variations in V-O interatomic distances, 26 or coordination environment. 27,28 The extended X-ray absorption fine structure (EXAFS), Fig. 2b showed a shift in the first V-O peak to a larger distance, and a contraction of the second shell V-V/V-O peak.…”
Section: Resultsmentioning
confidence: 99%
“…52,53 The shoulder M 1 at 8.992 eV and the peak M 2 at 8.997 eV are assigned respectively to the 1s4pz and to the 1s 4px,y transitions. The broad peak B around 9 eV is caused by multiple scattering of the photoelectron within the first coordination shell of Cu II 54,55 so that its energy position indirectly depends upon the Cu II -N bond length. Long under debate, the assignment of peak S at 8.985 keV was eventually ascertained through polarization-resolved XAS experiments 56 and ab-initio calculations.…”
Section: Spectroscopic Characterizations Of Cumentioning
confidence: 99%