TY - JOUR
T1 - Magnetic and transport properties of YBNIGe with a TiNiSi-type structure
AU - Araki, Koji
AU - Kohei, Takeru
AU - Tanaka, Hiroki
AU - Nakamura, Shintaro
AU - Nojima, Tsutomu
AU - Ochiai, Akira
AU - Katoh, Kenichi
N1 - Publisher Copyright:
©2019 The Physical Society of Japan
PY - 2019
Y1 - 2019
N2 - The magnetic and transport properties of a single crystal of YbNiGe with an orthorhombic TiNiSi-type structure are presented here. The experimental results indicate that YbNiGe undergoes two successive antiferromagnetic transitions at TN = 3.6K and Tm = 3.0K at zero field. The magnetic susceptibility and magnetization for the three principal axes show large anisotropy with the magnetic easy-axis along the a-axis, reflecting the orthorhombic crystal structure. The electrical resistivity for the current along the three principal axes shows a metallic behavior with a Kondo increase below around 50K. The magnetic entropy released at TN is 54% of Rln2 for the Kramers doublet ground state. The Sommerfeld coefficient γ is estimated to be 83.3mJ=mol K2 below 1K. The obtained value of A=γ2, where A is the coefficient of the T2 dependence of the resistivity at low temperatures, is larger than the universal value of the Kadowaki–Woods relation for heavy-fermion systems, i.e., A=γ2 = 1.0 × 10−5µΩ·cm(mol·K=mJ)2. Furthermore, this paper discusses the possible nature of two successive antiferromagnetic transitions of YbNiGe in comparison with related isostructural YbTGe compounds.
AB - The magnetic and transport properties of a single crystal of YbNiGe with an orthorhombic TiNiSi-type structure are presented here. The experimental results indicate that YbNiGe undergoes two successive antiferromagnetic transitions at TN = 3.6K and Tm = 3.0K at zero field. The magnetic susceptibility and magnetization for the three principal axes show large anisotropy with the magnetic easy-axis along the a-axis, reflecting the orthorhombic crystal structure. The electrical resistivity for the current along the three principal axes shows a metallic behavior with a Kondo increase below around 50K. The magnetic entropy released at TN is 54% of Rln2 for the Kramers doublet ground state. The Sommerfeld coefficient γ is estimated to be 83.3mJ=mol K2 below 1K. The obtained value of A=γ2, where A is the coefficient of the T2 dependence of the resistivity at low temperatures, is larger than the universal value of the Kadowaki–Woods relation for heavy-fermion systems, i.e., A=γ2 = 1.0 × 10−5µΩ·cm(mol·K=mJ)2. Furthermore, this paper discusses the possible nature of two successive antiferromagnetic transitions of YbNiGe in comparison with related isostructural YbTGe compounds.
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U2 - 10.7566/JPSJ.88.114709
DO - 10.7566/JPSJ.88.114709
M3 - Article
AN - SCOPUS:85074791871
SN - 0031-9015
VL - 88
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 11
M1 - 114709
ER -