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 - 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.
UR - http://www.scopus.com/inward/record.url?scp=85131964371&partnerID=8YFLogxK
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 -