TY - JOUR
T1 - Electronic Structure of Spinel-Type MgTi2O4
T2 - Valence Change at Surface and Effect of Fe Substitution for Mg
AU - Yamaguchi, Tomoyuki
AU - Okawa, Mario
AU - Wadati, Hiroki
AU - Regier, Tom Z.
AU - Saitoh, Tom
AU - Takagi, Yasumasa
AU - Yasui, Akira
AU - Isobe, Masahiko
AU - Ueda, Yutaka
AU - Mizokawa, Takashi
N1 - Funding Information:
Acknowledgements The XAS measurements reported in this paper were performed at the Canadian Light Source, a national research facility of the University of Saskatchewan, which is supported by the Canada Foundation for Innovation (CFI), the Natural Sciences and Engineering Research Council (NSERC), the National Research Council (NRC), the Canadian Institutes of Health Research (CIHR), the Government of Saskatchewan, and the University of Saskatchewan. The HAXPES measurements were performed with the approval of SPring-8 (2018B1021 and 2018B1049). This work was partially supported by CREST-JST (Grant No. JPMJCR15Q2) and KAKENHI from JSPS (Grants Nos. JP19H01853 and JP19H00659).
Funding Information:
The XAS measurements reported in this paper were performed at the Canadian Light Source, a national research facility of the University of Saskatchewan, which is supported by the Canada Foundation for Innovation (CFI), the Natural Sciences and Engineering Research Council (NSERC), the National Research Council (NRC), the Canadian Institutes of Health Research (CIHR), the Government of Saskatchewan, and the University of Saskatchewan. The HAXPES measurements were performed with the approval of SPring-8 (2018B1021 and 2018B1049). This work was partially supported by CREST-JST (Grant No. JPMJCR15Q2) and KAKENHI from JSPS (Grants Nos. JP19H01853 and JP19H00659).
Publisher Copyright:
©2022 The Physical Society of Japan
PY - 2022/7/15
Y1 - 2022/7/15
N2 - Bulk and surface electronic states of MgTi2O4 have been investigated by means of x-ray absorption spectroscopy (XAS), hard x-ray photoemission spectroscopy (HAXPES), and theoretical calculations. The Ti 2p XAS spectra exhibit multiplet structures derived from the bulk Ti3+ and surface Ti4+ features. In the surface sensitive O 1s XAS of the total electron yield mode, the magnitude of ligand field splitting is enhanced due to existence of surface Ti4+ species. The bulk-sensitive O 1s XAS spectrum taken in the total fluorescence yield mode is well reproduced by unoccupied part of O 2p density of states obtained by band structure calculations with on-site Coulomb interaction U for Ti 3d. In addition, occupied part of the calculated Ti 3d density of states agrees with the hard x-ray photoemission spectrum indicating Mottness of Ti 3d electrons. In Mg1−xFexTi2O4, the bulk sensitive Fe 2p XAS is consistent with high spin Fe2+ indicating isovalent substitution for Mg while the surface sensitive Fe 2p XAS includes high spin Fe3+. The multiplet structures in the Ti 2p and Fe 2p XAS spectra show that the 3d electrons in the bulk Ti3+ and Fe2+ are basically localized. On the other hand, a low energy shoulder of the Ti 2p HAXPES peak, which can be assigned to Ti2+ or screening effect, suggests charge fluctuation due to proximity to the metal–insulator transition.
AB - Bulk and surface electronic states of MgTi2O4 have been investigated by means of x-ray absorption spectroscopy (XAS), hard x-ray photoemission spectroscopy (HAXPES), and theoretical calculations. The Ti 2p XAS spectra exhibit multiplet structures derived from the bulk Ti3+ and surface Ti4+ features. In the surface sensitive O 1s XAS of the total electron yield mode, the magnitude of ligand field splitting is enhanced due to existence of surface Ti4+ species. The bulk-sensitive O 1s XAS spectrum taken in the total fluorescence yield mode is well reproduced by unoccupied part of O 2p density of states obtained by band structure calculations with on-site Coulomb interaction U for Ti 3d. In addition, occupied part of the calculated Ti 3d density of states agrees with the hard x-ray photoemission spectrum indicating Mottness of Ti 3d electrons. In Mg1−xFexTi2O4, the bulk sensitive Fe 2p XAS is consistent with high spin Fe2+ indicating isovalent substitution for Mg while the surface sensitive Fe 2p XAS includes high spin Fe3+. The multiplet structures in the Ti 2p and Fe 2p XAS spectra show that the 3d electrons in the bulk Ti3+ and Fe2+ are basically localized. On the other hand, a low energy shoulder of the Ti 2p HAXPES peak, which can be assigned to Ti2+ or screening effect, suggests charge fluctuation due to proximity to the metal–insulator transition.
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U2 - 10.7566/JPSJ.91.074704
DO - 10.7566/JPSJ.91.074704
M3 - Article
AN - SCOPUS:85131964371
SN - 0031-9015
VL - 91
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 7
M1 - 074704
ER -