TY - JOUR
T1 - Anisotropy of magnetization and specific heat of TmTi2Al20 single crystal
AU - Namiki, Takahiro
AU - Matsumoto, Yuki
AU - Isikawa, Yosikazu
AU - Nishimura, Katsuhiko
N1 - Publisher Copyright:
© 2021 The Physical Society of Japan
PY - 2021/11/15
Y1 - 2021/11/15
N2 - The magnetization M, magnetic susceptibility M=H, and specific heat C of TmTi2Al20 single crystal have been measured in an external magnetic field along the crystalline principal directions, [001], [101], and [111], at temperatures down to 0.5 K. Antiferromagnetic transition was observed at 0.62 K in both M(T)=H and C(T) curves. The metamagnetic transitions were detected at the critical field Hc ranging from 0.12 to 0.16 T depending on the field direction. M(H) curves at 0.5 K showed a large magnetic anisotropy, revealing that the hard and easy axes of magnetization were along the [001] and [111] directions below approximately 4 T, respectively, but above the critical field, the easy axis changed to the [101] direction. The observed C(T) peaks appeared remarkably sharp below Hc, being almost independent of the field direction. The peak heights and positions in the C(T) curves were substantially decreased by a small external field. The C(T) curves above Hc, in contrast, showed anisotropic behaviors depending on the field direction. These anisotropies observed in M(T)=H, M(H), and C(T) were analyzed by taking into account the crystalline-field effect, Zeeman effect, and magnetic exchange interactions.
AB - The magnetization M, magnetic susceptibility M=H, and specific heat C of TmTi2Al20 single crystal have been measured in an external magnetic field along the crystalline principal directions, [001], [101], and [111], at temperatures down to 0.5 K. Antiferromagnetic transition was observed at 0.62 K in both M(T)=H and C(T) curves. The metamagnetic transitions were detected at the critical field Hc ranging from 0.12 to 0.16 T depending on the field direction. M(H) curves at 0.5 K showed a large magnetic anisotropy, revealing that the hard and easy axes of magnetization were along the [001] and [111] directions below approximately 4 T, respectively, but above the critical field, the easy axis changed to the [101] direction. The observed C(T) peaks appeared remarkably sharp below Hc, being almost independent of the field direction. The peak heights and positions in the C(T) curves were substantially decreased by a small external field. The C(T) curves above Hc, in contrast, showed anisotropic behaviors depending on the field direction. These anisotropies observed in M(T)=H, M(H), and C(T) were analyzed by taking into account the crystalline-field effect, Zeeman effect, and magnetic exchange interactions.
UR - http://www.scopus.com/inward/record.url?scp=85117462306&partnerID=8YFLogxK
U2 - 10.7566/JPSJ.90.114602
DO - 10.7566/JPSJ.90.114602
M3 - 学術論文
AN - SCOPUS:85117462306
SN - 0031-9015
VL - 90
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 11
M1 - 114602
ER -