TY - JOUR
T1 - Anomalous hall effect of pyrochlore molybdate Nd2Mo2O7
AU - Yoshii, Shunsuke
AU - Iikubo, Satoshi
AU - Kageyama, Taketomo
AU - Oda, Keisuke
AU - Kondo, Yasuyuki
AU - Murata, Kazuhiro
AU - Sato, Masatoshi
PY - 2000/12
Y1 - 2000/12
N2 - Hall resistivity ρH has been investigated for single crystals of pyrochlore molybdate Nd2Mo2O7. With decreasing temperature T, the anomalous Hall effect appears at around the Curie temperature TC (∼95K). In the relatively high temperature region (T > 60K), ρH can be described by the well-known equation ρH = R0H + 4πRsM, where R0 and Rs are the ordinary and anomalous Hall coefficients, respectively, and M is the net magnetization predominantly contributed by the Mo spins. With further decreasing T, the ordering of the Nd moments, which is confirmed by neutron diffraction studies carried out by the present authors' group, induces marked change in the behavior of the anomalous part of ρH. The behavior in the low temperature region has been found to be simply described by the equation ρH = R0H + 4πRsMMo + 4πR′sMNd, where MMo and MNd are the net magnetizations of the Mo- and Nd-moments, respectively. This result and the T-dependence of Rs and R′s are quite different from those known for ordinary ferromagnets and might be related to the nonzero spin chirality observed in the present system.
AB - Hall resistivity ρH has been investigated for single crystals of pyrochlore molybdate Nd2Mo2O7. With decreasing temperature T, the anomalous Hall effect appears at around the Curie temperature TC (∼95K). In the relatively high temperature region (T > 60K), ρH can be described by the well-known equation ρH = R0H + 4πRsM, where R0 and Rs are the ordinary and anomalous Hall coefficients, respectively, and M is the net magnetization predominantly contributed by the Mo spins. With further decreasing T, the ordering of the Nd moments, which is confirmed by neutron diffraction studies carried out by the present authors' group, induces marked change in the behavior of the anomalous part of ρH. The behavior in the low temperature region has been found to be simply described by the equation ρH = R0H + 4πRsMMo + 4πR′sMNd, where MMo and MNd are the net magnetizations of the Mo- and Nd-moments, respectively. This result and the T-dependence of Rs and R′s are quite different from those known for ordinary ferromagnets and might be related to the nonzero spin chirality observed in the present system.
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U2 - 10.1143/JPSJ.69.3777
DO - 10.1143/JPSJ.69.3777
M3 - Article
AN - SCOPUS:0034556940
SN - 0031-9015
VL - 69
SP - 3777
EP - 3780
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 12
ER -