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Crystal growth, transport, and magnetic properties of Ln3Co4Sn13 (Ln=La, Ce) with a perovskite-like structure
Authors:Evan Lyle Thomas  Andrew N Bankston  Peter Klavins  David P Young  Julia Y Chan
Institution:a Department of Chemistry, Louisiana State University, 232 Choppin Hall, Baton Rouge, LA 70803, USA
b Department of Physics, University of California, Davis, CA 95616, USA
c Department of Physics and Astronomy, Louisiana State University, Baton Rouge, LA 70803, USA
Abstract:Ln3Co4Sn13 (Ln=La, Ce) have been synthesized by flux growth and characterized by single crystal X-ray diffraction. These compounds adopt the Yb3Rh4Sn13-type structure and crystallize in the cubic space group View the MathML source (No. 223) with Z=2. Lattice parameters at 298 K are View the MathML source, View the MathML source, and View the MathML source, View the MathML source for the La and Ce analogues, respectively. The crystal structure consists of an Sn-centered icosahedron at the origin of the unit cell, which shares faces with eight Co trigonal prisms and 12 Ln-centered cuboctahedra. Magnetization data at 0.1 T show paramagnetic behavior down to 1.8 K for Ce3Co4Sn13, with View the MathML source per Ce3+, while conventional type II superconductivity appears below 2.85 K in the La compound. Electrical resistivity and specific heat data for the La compound show a corresponding sharp superconducting transition at Tc∼2.85 K. The entropy and resistivity data for Ce3Co4Sn13 show the existence of the Kondo effect with a complicated semiconducting-like behavior in the resistivity data. In addition, a large enhanced specific heat coefficient at low T with a low magnetic transition temperature suggests a heavy-fermionic character for the Ce compound. Herein, the structure and physical properties of Ln3Co4Sn13 (Ln=La, Ce) are discussed.
Keywords:Ce3Co4Sn13  La3Co4Sn13  Ln3Co4Sn13  SnLn3Co4Sn12  SnCe3Co4Sn12  X-ray diffraction  Electrical resistivity  Rare-earth cuboctahedra  Icosahedra  Rare-earth intermetallics  Stannides  Superconductivity  Specific heat  Heavy fermion
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