TY - JOUR
T1 - Interplay between Mott physics and Peierls physics in hollandite-type vanadates with a metal-insulator transition
AU - Ishige, Y.
AU - Sudayama, T.
AU - Wakisaka, Y.
AU - Mizokawa, T.
AU - Wadati, H.
AU - Sawatzky, G. A.
AU - Regier, T. Z.
AU - Isobe, M.
AU - Ueda, Y.
PY - 2011/3/22
Y1 - 2011/3/22
N2 - We report an x-ray photoemission spectroscopy (XPS) and x-ray absorption spectroscopy (XAS) study on K2V8-xTixO 16 (x=0.0, 0.3, and 4.0) in which the metal-insulator transition (MIT) and the tetragonal-to-monoclinic structural transition show different responses against the Ti doping. The spectral change of V 2p XAS across the MIT is similar to that observed in VO2, indicating that the V-V pairing is responsible for the MIT. In the insulating phase, the V 2p XPS spectra are split into the V3+ and V4+ features showing the localized character of the V 3d electrons. In addition, the V 2p XAS spectra of the monoclinic insulating phase suggest that the V-V pairing is weakened, and, instead, the V3+-V4+ coupling is strengthened by orbital ordering. In contrast to VO2, the existence of the V3+ component in K2V8-xTixO16 gives additional orbital instability in the insulating phase, which competes with the V-V pairing.
AB - We report an x-ray photoemission spectroscopy (XPS) and x-ray absorption spectroscopy (XAS) study on K2V8-xTixO 16 (x=0.0, 0.3, and 4.0) in which the metal-insulator transition (MIT) and the tetragonal-to-monoclinic structural transition show different responses against the Ti doping. The spectral change of V 2p XAS across the MIT is similar to that observed in VO2, indicating that the V-V pairing is responsible for the MIT. In the insulating phase, the V 2p XPS spectra are split into the V3+ and V4+ features showing the localized character of the V 3d electrons. In addition, the V 2p XAS spectra of the monoclinic insulating phase suggest that the V-V pairing is weakened, and, instead, the V3+-V4+ coupling is strengthened by orbital ordering. In contrast to VO2, the existence of the V3+ component in K2V8-xTixO16 gives additional orbital instability in the insulating phase, which competes with the V-V pairing.
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U2 - 10.1103/PhysRevB.83.125112
DO - 10.1103/PhysRevB.83.125112
M3 - Article
AN - SCOPUS:79961071140
SN - 0163-1829
VL - 83
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 12
M1 - 125112
ER -