TY - JOUR
T1 - Effect of pressure on the field-induced ordered phase in the heavy-fermion compound YbCo 2 Zn 20
AU - Takeuchi, Tetsuya
AU - Taga, Yuki
AU - Yoshiuchi, Shingo
AU - Ohya, Masahiro
AU - Hirose, Yusuke
AU - Honda, Fuminori
AU - Settai, Rikio
AU - Ōnuki, Yoshichika
N1 - Funding Information:
This work was supported by a Grant-in-Aid for Scientific Research on Innovative Areas Heavy Electrons (No. 20102002), Specially Promoted Research (No. 20001004), and Osaka University Global COE Program Core Research and Engineering of Advanced Materials-Interdisciplinary Education Center for Materials Science (G10) from the Ministry of Education, Culture, Sports, Science, and Technology, Japan.
PY - 2013/7
Y1 - 2013/7
N2 - The effect of pressure on the field-induced ordered phase for H {norm of matrix} 〈111〉 in the heavy-fermion compound YbCo 2 Zn 20 , which is presumably a field-induced antiferro-quadrupolar (FI-AFQ) phase, was investigated in the pressure range up to 4.5 GPa and under magnetic fields up to 80 kOe. When pressure is applied, the metamagnetic-like transition at H m =6 kOe shifts to lower fields and disappears around the quantum critical pressure P c ∼1.8 GPa. A pressure-induced antiferromagnetic (PI-AFM) phase appears at pressures above about 2 GPa, and the critical field H c of the PI-AFM phase increases with increasing pressure. On the other hand, the transition field H Q of the FI-AFQ phase decreases gradually without showing any anomalous behavior around P c and becomes obscure around 4 GPa, where H c of the PI-AFM phase and H Q of the FI-AFQ phase become comparable. The magnetic field versus pressure, H-P, phase diagram for H {norm of matrix} 〈111〉 at 0.1 K was constructed in the pressure range up to 4.5 GPa.
AB - The effect of pressure on the field-induced ordered phase for H {norm of matrix} 〈111〉 in the heavy-fermion compound YbCo 2 Zn 20 , which is presumably a field-induced antiferro-quadrupolar (FI-AFQ) phase, was investigated in the pressure range up to 4.5 GPa and under magnetic fields up to 80 kOe. When pressure is applied, the metamagnetic-like transition at H m =6 kOe shifts to lower fields and disappears around the quantum critical pressure P c ∼1.8 GPa. A pressure-induced antiferromagnetic (PI-AFM) phase appears at pressures above about 2 GPa, and the critical field H c of the PI-AFM phase increases with increasing pressure. On the other hand, the transition field H Q of the FI-AFQ phase decreases gradually without showing any anomalous behavior around P c and becomes obscure around 4 GPa, where H c of the PI-AFM phase and H Q of the FI-AFQ phase become comparable. The magnetic field versus pressure, H-P, phase diagram for H {norm of matrix} 〈111〉 at 0.1 K was constructed in the pressure range up to 4.5 GPa.
UR - http://www.scopus.com/inward/record.url?scp=84879996441&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84879996441&partnerID=8YFLogxK
U2 - 10.3938/jkps.62.1852
DO - 10.3938/jkps.62.1852
M3 - Article
AN - SCOPUS:84879996441
SN - 0374-4884
VL - 62
SP - 1852
EP - 1854
JO - Journal of the Korean Physical Society
JF - Journal of the Korean Physical Society
IS - 12
ER -