TY - JOUR
T1 - Weak Kondo Coupling Antiferromagnet CePd3Sn2 with Quasi-One-Dimensional Ce Chains
AU - Kawaue, Yudai
AU - Oishi, Ryohei
AU - Yang, Chongli
AU - Yamamoto, Rikako
AU - Shimura, Yasuyuki
AU - Umeo, Kazunori
AU - Onimaru, Takahiro
AU - Adroja, Devashibhai T.
AU - Walker, Helen C.
AU - Takabatake, Toshiro
N1 - Publisher Copyright:
© 2024 The Physical Society of Japan.
PY - 2024/3
Y1 - 2024/3
N2 - CePd3Sn2 with Ce-chains along the orthorhombic b axis has been reported to order antiferromagnetically at TN ∼ 0.6 K. Above TN, the specific heat C(T) exhibits a long tail whose origin remains elusive. Here we report on the physical properties of single-crystalline samples inferred from electrical resistivity ρ(T), magnetization M(B), and C(T). The measurements reveal rather weak anisotropic properties characterized by the lowest ρ(T) and the highest saturation M(B) along the b axis. The ρ(T) data along the three principal directions exhibit no clear signature of Kondo scattering and decrease with negative curvatures on cooling from 2K to TN = 0.67 K. The magnetic susceptibility and inelastic neutron scattering data are reproduced by the crystal electric field (CEF) model for the Ce3+ ion with two excited CEF doublets at rather low energies 27 and 191 K, respectively, above the ground state doublet. The isothermal M(B) curves at 0.3K show metamagnetic transitions at B ∥ b = 1.8 T and B ∥ c = 1.5 T and upward increases before saturation for the three directions. The antiferromagnetic order is destroyed by the application of magnetic field in an anisotropic way at around B ∥ b = 3T, B ∥ c = 4 T, and B ∥ a = 5 T. The obtained results are discussed by comparing with those reported for quasi-one-dimensional Ce compounds.
AB - CePd3Sn2 with Ce-chains along the orthorhombic b axis has been reported to order antiferromagnetically at TN ∼ 0.6 K. Above TN, the specific heat C(T) exhibits a long tail whose origin remains elusive. Here we report on the physical properties of single-crystalline samples inferred from electrical resistivity ρ(T), magnetization M(B), and C(T). The measurements reveal rather weak anisotropic properties characterized by the lowest ρ(T) and the highest saturation M(B) along the b axis. The ρ(T) data along the three principal directions exhibit no clear signature of Kondo scattering and decrease with negative curvatures on cooling from 2K to TN = 0.67 K. The magnetic susceptibility and inelastic neutron scattering data are reproduced by the crystal electric field (CEF) model for the Ce3+ ion with two excited CEF doublets at rather low energies 27 and 191 K, respectively, above the ground state doublet. The isothermal M(B) curves at 0.3K show metamagnetic transitions at B ∥ b = 1.8 T and B ∥ c = 1.5 T and upward increases before saturation for the three directions. The antiferromagnetic order is destroyed by the application of magnetic field in an anisotropic way at around B ∥ b = 3T, B ∥ c = 4 T, and B ∥ a = 5 T. The obtained results are discussed by comparing with those reported for quasi-one-dimensional Ce compounds.
UR - http://www.scopus.com/inward/record.url?scp=85188215432&partnerID=8YFLogxK
U2 - 10.7566/JPSJ.93.034706
DO - 10.7566/JPSJ.93.034706
M3 - Article
AN - SCOPUS:85188215432
SN - 0031-9015
VL - 93
SP - 1
EP - 7
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 3
ER -