Nonmagnetic ground state, Crystal field effects and Heavy-fermion behaviour in the Remeika Phase: Pr$_3$Ir$_4$Ge$_{13}$

TL;DR

This study investigates Pr$_3$Ir$_4$Ge$_{13}$, revealing a nonmagnetic ground state, crystal field effects, and moderate heavy-fermion behavior, with complex transport properties and no phase transition down to 1.9 K.

Contribution

It provides detailed experimental insights into the magnetic, electronic, and thermal properties of Pr$_3$Ir$_4$Ge$_{13}$, highlighting its crystal field singlet ground state and heavy-fermion characteristics.

Findings

Pr$_3$Ir$_4$Ge$_{13}$ has a crystal electric field singlet ground state.

The compound exhibits a negative temperature coefficient of resistivity.

It shows moderate heavy-fermion behavior with a large Sommerfeld coefficient.

Abstract

We report the magnetic, electronic and transport properties of the quasi-skutterudite compound Pr$_3$Ir$_4$Ge$_{13}$ by means of magnetic susceptibility $\chi(T)$, electrical resistivity $\rho(T)$, specific heat $C_p(T)$, thermal conductivity $\kappa(T)$, thermoelectric power $S(T)$ and Hall coefficient $R_\mathrm{H}(T)$ measurements. Pr$_3$Ir$_4$Ge$_{13}$ does not show any phase transition down to 1.9 K. Magnetic, and specific measurements show that the system possesses a crystal electric field singlet ground state that is separated from the first excited state by about 37 K. $\rho(T)$ shows a negative temperature coefficient of resistance for the whole temperature range studied and which can be explained in terms of Mott's impurity band conduction mechanism. $R_\mathrm{H}(T)$ measurements show that Pr$_3$Ir$_4$Ge$_{13}$ is a low-carrier density semimetal and its transport properties indicate a metallic-non metallic cross over behaviour. Large Seebeck values were observed for the entire temperature range of investigation, and the analysis of temperature variation of $S$ and $S/T$ showed no sign of strong correlation between the Pr 4$f^2$ and conduction electron states near Fermi level. A large Sommerfeld coefficient, $\gamma = 150$~mJ/(mol K$^2$) indicates the formation of a moderate heavy-fermion state emerging from the dynamical crystal field fluctuations.