TY - JOUR
T1 - Magnetization process of itinerant-electron-type helical-spin-glass reentrant magnet Cr0.81Mn0.19Ge observed on various spatial scales
AU - Sato, T.
AU - Furusaka, M.
AU - Takeda, M.
N1 - Funding Information:
One of the authors (T.S.) wishes to thank Dr. T. Taniyama of Tokyo Institute of Technology and Dr. T. Oku of the Institute of Physical and Chemical Research for their assistance in performing the experiments in the present study. The present study was supported in part by a Grant-in-Aid for Science Research from the Ministry of Education, Science and Culture. Additional support was provided by the Seki Foundation for the Promotion of Science and Technology, and by the Iketani Science and Technology Foundation.
PY - 1999/5
Y1 - 1999/5
N2 - The magnetization process of an itinerant-electron-type helical-spin-glass reentrant magnet Cr1-xMnxGe was analyzed using magnetic measurement, neutron depolarization analysis and small-angle neutron scattering, each of which has a different spatial resolution. At temperatures ranging from approx. 8 to 13 K, the helical magnetism having a wave vector parallel to the crystal axis is stable in a zero magnetic field. As the magnitude of the field increases, the conical spin structure having a screw axis parallel to the applied field appears, and the cone angle decreases continuously. This change in spin structure primarily determines the macroscopic magnetization process in low magnetic fields. Although a ferromagnetic structure is induced in higher applied fields, magnetization saturation is difficult to achieve due to the inter-domain interaction. At approximately 8 K, spin-glass-like singularity is confirmed by means of the above-mentioned experimental methods. The appearance of spin-glass-like behavior is accompanied by changes in spin configuration on a microscopic scale. This behavior can be interpreted in terms of a mean-field-type picture, based on the spatial scale of the interaction.
AB - The magnetization process of an itinerant-electron-type helical-spin-glass reentrant magnet Cr1-xMnxGe was analyzed using magnetic measurement, neutron depolarization analysis and small-angle neutron scattering, each of which has a different spatial resolution. At temperatures ranging from approx. 8 to 13 K, the helical magnetism having a wave vector parallel to the crystal axis is stable in a zero magnetic field. As the magnitude of the field increases, the conical spin structure having a screw axis parallel to the applied field appears, and the cone angle decreases continuously. This change in spin structure primarily determines the macroscopic magnetization process in low magnetic fields. Although a ferromagnetic structure is induced in higher applied fields, magnetization saturation is difficult to achieve due to the inter-domain interaction. At approximately 8 K, spin-glass-like singularity is confirmed by means of the above-mentioned experimental methods. The appearance of spin-glass-like behavior is accompanied by changes in spin configuration on a microscopic scale. This behavior can be interpreted in terms of a mean-field-type picture, based on the spatial scale of the interaction.
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U2 - 10.1016/S0304-8853(99)00181-X
DO - 10.1016/S0304-8853(99)00181-X
M3 - Article
AN - SCOPUS:0032655043
SN - 0304-8853
VL - 195
SP - 345
EP - 361
JO - Journal of Magnetism and Magnetic Materials
JF - Journal of Magnetism and Magnetic Materials
IS - 2
ER -