TY - JOUR
T1 - Ferromagnetism and giant magnetoresistance in the rare-earth fullerides (formula presented)
AU - Ishii, Kenji
AU - Fujiwara, Akihiko
AU - Suematsu, Hiroyoshi
AU - Kubozono, Yoshihiro
N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 2002
Y1 - 2002
N2 - We have studied crystal structure, magnetism, and electric transport properties of a europium fulleride (formula presented) and its Sr-substituted compounds, (formula presented) They have a bcc structure, which is an isostructure of other (formula presented) (formula presented) represents an alkali atom or an alkaline-earth atom). Magnetic measurements revealed that magnetic moment is ascribed to the divalent europium atom with (formula presented) spin, and a ferromagnetic transition was observed at (formula presented) In (formula presented) we also confirm the ferromagnetic transition by heat-capacity measurement. The striking feature in (formula presented) is very large negative magnetoresistance at low temperature; the resistivity ratio (formula presented) reaches almost (formula presented) at 1 K in (formula presented) Such large magnetoresistance is the manifestation of a strong (formula presented) interaction between conduction carriers on (formula presented) and (formula presented)(formula presented) electrons of Eu.
AB - We have studied crystal structure, magnetism, and electric transport properties of a europium fulleride (formula presented) and its Sr-substituted compounds, (formula presented) They have a bcc structure, which is an isostructure of other (formula presented) (formula presented) represents an alkali atom or an alkaline-earth atom). Magnetic measurements revealed that magnetic moment is ascribed to the divalent europium atom with (formula presented) spin, and a ferromagnetic transition was observed at (formula presented) In (formula presented) we also confirm the ferromagnetic transition by heat-capacity measurement. The striking feature in (formula presented) is very large negative magnetoresistance at low temperature; the resistivity ratio (formula presented) reaches almost (formula presented) at 1 K in (formula presented) Such large magnetoresistance is the manifestation of a strong (formula presented) interaction between conduction carriers on (formula presented) and (formula presented)(formula presented) electrons of Eu.
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U2 - 10.1103/PhysRevB.65.134431
DO - 10.1103/PhysRevB.65.134431
M3 - Article
AN - SCOPUS:85038323434
SN - 1098-0121
VL - 65
SP - 1
EP - 6
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 13
ER -