TY - JOUR
T1 - Photoemission study of the metal-insulator transition
AU - Mamiya, K.
AU - Mizokawa, T.
AU - Fujimori, A.
AU - Miyadai, T.
PY - 1998
Y1 - 1998
N2 - We have studied the electronic structure of (Formula presented) which undergoes a metal-insulator transition as functions of composition (Formula presented) and temperature, by means of photoemission and inverse-photoemission spectroscopy. Spectral changes across the transition near the Fermi level (Formula presented) (particularly within (Formula presented) of (Formula presented) have been interpreted as due to a “semimetallic” closure of the band gap in going from the insulating phase to the antiferromagnetic metallic phase. On the other hand, there is also composition- and temperature-dependent spectral weight transfer over a wider energy range of (Formula presented) indicating significant correlation effects. Photoemission intensity just below (Formula presented) remains high in the insulating phases, indicating that the carrier number is large at high temperatures and that the activation-type transport is due to the activated mobility rather than the activated carrier number.
AB - We have studied the electronic structure of (Formula presented) which undergoes a metal-insulator transition as functions of composition (Formula presented) and temperature, by means of photoemission and inverse-photoemission spectroscopy. Spectral changes across the transition near the Fermi level (Formula presented) (particularly within (Formula presented) of (Formula presented) have been interpreted as due to a “semimetallic” closure of the band gap in going from the insulating phase to the antiferromagnetic metallic phase. On the other hand, there is also composition- and temperature-dependent spectral weight transfer over a wider energy range of (Formula presented) indicating significant correlation effects. Photoemission intensity just below (Formula presented) remains high in the insulating phases, indicating that the carrier number is large at high temperatures and that the activation-type transport is due to the activated mobility rather than the activated carrier number.
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U2 - 10.1103/PhysRevB.58.9611
DO - 10.1103/PhysRevB.58.9611
M3 - Article
AN - SCOPUS:0006076632
VL - 58
SP - 9611
EP - 9614
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
SN - 0163-1829
IS - 15
ER -