Crystal structure and physical properties of the two stannides EuPdSn2 and YbPdSn2

We report on synthesis, crystal structure and physical properties of the isotypic compounds YbPdSn2 and EuPdSn2 crystallizing in the MgCuAl2-type structure. In both stannides a divalent state of respective rare earth element was found from analysis of the magnetic susceptibilities. Whereas in YbPdSn2 only weak paramagnetic behaviour is observed, in EuPdSn2 a long-range magnetic phase transition occurs at 12.5 K with complex magnetic behaviour evidenced by magnetic susceptibity and specific heat measurements. Under the influence of magnetic field, the magnetic behaviour was found to evolve from an antiferromagnetic to a ferromagnetic state as a consequence of a re-arrangement of magnetic moments.

[1]  P. Skyba,et al.  YbPd$_2$In: a promising candidate to strong entropy accumulation at very low temperature , 2017 .

[2]  M. Giovannini,et al.  Crystal structure and magnetic properties of new Eu-Pd-Sn compounds , 2017 .

[3]  A. Saccone,et al.  Isothermal section at 600 °C of the Yb−Pd−Sn system (Pd ≤ 75 at.%) , 2017 .

[4]  F. Steglich,et al.  Foundations of heavy-fermion superconductivity: lattice Kondo effect and Mott physics , 2016, Reports on progress in physics. Physical Society.

[5]  G. Ehlers,et al.  Orbital-exchange and fractional quantum number excitations in an f-electron metal, Yb2Pt2Pb , 2016, Science.

[6]  A. P. Gonçalves,et al.  Magnetic properties of the selected phases from the Eu–Ag–Al and Eu–Ag–Ga systems , 2015 .

[7]  R. Pöttgen,et al.  The Stannides EuPd2Sn2, EuPt2Sn2, EuAu2Sn2, and Eu5.4Sn5.6 – Structure and Magnetic Properties , 2014 .

[8]  J. Cadogan,et al.  The magnetic structure of EuPdSn. , 2012, Journal of physics. Condensed matter : an Institute of Physics journal.

[9]  D. Ryan,et al.  Structural and physical properties of the new intermetallic compound Yb{sub 3}Pd{sub 2}Sn{sub 2} , 2011 .

[10]  K. Shimizu,et al.  Reentrant quantum criticality in Yb2Pd2Sn , 2011 .

[11]  A. Saccone,et al.  Phase relationships at 600 °C of the Yb–Pd–Sn system from 25 to 100 at.% Yb , 2010 .

[12]  C. Baines,et al.  Magnetic-field-induced crossover from non-Fermi to Fermi liquid at the quantum critical point of YbCu 5-x Au x , 2008, 0809.2685.

[13]  H. Sato,et al.  The magnetic instability of Yb2Pd2(In,Sn) in a non-Fermi liquid environment , 2005 .

[14]  Z. Kang,et al.  Binary rare earth oxides , 2005 .

[15]  M. Giovannini,et al.  Dynamical susceptibility and magnetic-field effect at the quantum critical point in CeCu 6 − x Au x from Cu NQR-NMR relaxation , 2003 .

[16]  R. Pöttgen,et al.  Notizen: Synthesis and Structure of YbPdSn2 , 2001 .

[17]  H. Eckert,et al.  A 119Sn and 151Eu Mössbauerspectroscopic, magnetic susceptibility, and electrical conductivity investigationof the stannides EuTSn (T = Cu, Pd, Ag, Pt) , 2001 .

[18]  R. Pöttgen,et al.  EuPdIn2, YbPdIn2, and YbAuIn2: Syntheses, Structures, and Properties of New Intermetallic Compounds with Ordered Re3B‐Type Structure , 1999 .

[19]  G. Nolze,et al.  POWDER CELL– a program for the representation and manipulation of crystal structures and calculation of the resulting X‐ray powder patterns , 1996 .

[20]  Juan Rodríguez-Carvajal,et al.  Recent advances in magnetic structure determination by neutron powder diffraction , 1993 .

[21]  Malik,et al.  Magnetic-susceptibility and electrical-resistivity measurements on RPdSn (R=Ce-Yb) compounds. , 1992, Physical review. B, Condensed matter.

[22]  J. Eisenstein Superconducting elements. [Review] , 1954 .