TY - JOUR
T1 - Not a Simple Ferro-quadrupole Order in DyB6
AU - Sera, Masafumi
AU - Yonemura, Takumi
AU - Itamochi, Ken
AU - Matsumura, Takeshi
AU - Hiroi, Masahiko
AU - Takahashi, Kohki
N1 - Publisher Copyright:
©2019 The Physical Society of Japan
PY - 2019
Y1 - 2019
N2 - We performed detailed measurements of the thermal and magnetic properties in the ferroquadrupole (FQ) ordered state of DyB6, which exhibits the antiferromagnetic (AFM) order at TN = 26 K and the O2 0½111 -type FQ order at TQ = 32 K. We also performed the mean-field calculation for the two-sublattice model in which the crystalline electric field (CEF) effect and AFM and FQ interactions are taken into account, focusing on the FQ ordered state. We could estimate the CEF level scheme to reproduce the temperature dependence of the magnetic susceptibility and specific heat. We could also reproduce the temperature dependence of the specific heat in the ordered state by the calculation quite well. However, the thermal and magnetic properties in magnetic fields, i.e., a decrease in the magnetic susceptibility below TQ, a nearly temperature-independent behavior of the electrical resistivity between TN and TQ, the magnetic phase diagram for H ∥ [111] and so forth could not be reproduced by the calculation where the dependence of the domain distribution on the magnetic field direction is taken into account.
AB - We performed detailed measurements of the thermal and magnetic properties in the ferroquadrupole (FQ) ordered state of DyB6, which exhibits the antiferromagnetic (AFM) order at TN = 26 K and the O2 0½111 -type FQ order at TQ = 32 K. We also performed the mean-field calculation for the two-sublattice model in which the crystalline electric field (CEF) effect and AFM and FQ interactions are taken into account, focusing on the FQ ordered state. We could estimate the CEF level scheme to reproduce the temperature dependence of the magnetic susceptibility and specific heat. We could also reproduce the temperature dependence of the specific heat in the ordered state by the calculation quite well. However, the thermal and magnetic properties in magnetic fields, i.e., a decrease in the magnetic susceptibility below TQ, a nearly temperature-independent behavior of the electrical resistivity between TN and TQ, the magnetic phase diagram for H ∥ [111] and so forth could not be reproduced by the calculation where the dependence of the domain distribution on the magnetic field direction is taken into account.
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U2 - 10.7566/JPSJ.88.054703
DO - 10.7566/JPSJ.88.054703
M3 - Article
AN - SCOPUS:85067254014
SN - 0031-9015
VL - 88
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 5
M1 - 054703
ER -