Antiferromagnetic ordering in the Kondo lattice system Yb$_2$Fe$_3$Si$_5$
Yogesh Singh, S.Ramakrishnan (Tata Institute for Fundamental Research,, Mumbai, India) Z.Hossain, C.Geibel (Max Planck Institute for the Chemical, Physics of Solids, Dresden, Germany)

TL;DR
This study investigates the magnetic and electronic properties of Yb$_2$Fe$_3$Si$_5$, revealing antiferromagnetic ordering below 1.7 K and Kondo lattice behavior with a large Sommerfeld coefficient, without superconductivity at low temperatures.
Contribution
It provides the first comprehensive bulk property analysis of Yb$_2$Fe$_3$Si$_5$, highlighting its antiferromagnetic order and Kondo lattice characteristics.
Findings
Yb$^{3+}$ moments order antiferromagnetically below 1.7 K
Yb$_2$Fe$_3$Si$_5$ exhibits Kondo lattice behavior with large Sommerfeld coefficient
No superconductivity observed down to 0.3 K at ambient pressure
Abstract
Compounds belonging to the RFeSi series exhibit unusual superconducting and magnetic properties. Although a number of studies have been made on the first reentrant antiferromagnet superconductor TmFeSi, the physical properties of YbFeSi are largely unexplored. In this work, we attempt to provide a comprehensive study of bulk properties such as, resistivity, susceptibility and heat-capacity of a well characterized polycrystalline YbFeSi. Our measurements indicate that Yb moments order antiferromagnetically below 1.7 K. Moreover, the system behaves as a Kondo lattice with large Sommerfeld coefficient () of 0.5~J/Yb mol K at 0.3 K, which is well below T. The absence of superconductivity in YbFeSi down to 0.3 K at ambient pressure is attributed to the presence of the Kondo effect.
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