TY - JOUR
T1 - ∼8 keV photoemission of the metal-insulator transition system VO 2
AU - Suga, S.
AU - Sekiyama, A.
AU - Imada, S.
AU - Miyamachi, T.
AU - Fujiwara, H.
AU - Yamasaki, A.
AU - Yoshimura, K.
AU - Okada, K.
AU - Yabashi, M.
AU - Tamasaku, K.
AU - Higashiya, A.
AU - Ishikawa, T.
PY - 2009/10/5
Y1 - 2009/10/5
N2 - Hard and soft x-ray photoelectron spectroscopies (called HAXPES and SXPES) were performed at ∼8 and ∼1.25keV for the metal-insulator transitions (MIT) system VO2. From the sharp difference between HAXPES and SXPES in the O Is spectra, it was found that the clean surface of the metal VO 2 is covered with a less itinerant surface layer. Clear changes of the spectral shapes were observed in HAXPES on MIT for the V Is, 2p, 3s, 3p and O 1s core levels. The enhanced intensity of these core levels in the low-binding-energy (EB) region of the main peak in the metal phase is due to the non-local or long range screening effects. The V 3d valence band in the metal phase is composed of coherent and incoherent parts. The prominent peak near 0.9 eV in the insulator phase has an incoherent tail in the high-E B region and the peak and its lower EB components are understood to have a noticeable coherent component. It is experimentally confirmed that both electron correlation and band changes induced by lattice distortion are responsible for the spectral changes on MIT in VO2.
AB - Hard and soft x-ray photoelectron spectroscopies (called HAXPES and SXPES) were performed at ∼8 and ∼1.25keV for the metal-insulator transitions (MIT) system VO2. From the sharp difference between HAXPES and SXPES in the O Is spectra, it was found that the clean surface of the metal VO 2 is covered with a less itinerant surface layer. Clear changes of the spectral shapes were observed in HAXPES on MIT for the V Is, 2p, 3s, 3p and O 1s core levels. The enhanced intensity of these core levels in the low-binding-energy (EB) region of the main peak in the metal phase is due to the non-local or long range screening effects. The V 3d valence band in the metal phase is composed of coherent and incoherent parts. The prominent peak near 0.9 eV in the insulator phase has an incoherent tail in the high-E B region and the peak and its lower EB components are understood to have a noticeable coherent component. It is experimentally confirmed that both electron correlation and band changes induced by lattice distortion are responsible for the spectral changes on MIT in VO2.
UR - http://www.scopus.com/inward/record.url?scp=70749098695&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=70749098695&partnerID=8YFLogxK
U2 - 10.1088/1367-2630/11/10/103015
DO - 10.1088/1367-2630/11/10/103015
M3 - Article
AN - SCOPUS:70749098695
SN - 1367-2630
VL - 11
JO - New Journal of Physics
JF - New Journal of Physics
M1 - 103015
ER -