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We report thermal expansion and magnetostriction of the cubic non-Kramers system PrIr$_2$Zn$_{20}$ with a non-magnetic $varGamma_{3}$ ground state doublet. In previous experiments, antiferroquadrupolar order at hbox{$T_{mathrm{Q}}=0.11$,K} and a Fermi liquid state around $B_{mathrm{c}}approx5$,T for hbox{$boldsymbol{B}parallel[001]$}, indicative of possible ferrohastatic order, were discovered. For magnetic fields hbox{$boldsymbol{B}parallel[001]$}, the low temperature longitudinal and transverse thermal expansion and magnetostriction are highly anisotropic. The resulting volume strain is very small, indicating that the Pr valence remains nearly constant as a function of magnetic field. We conclude that the Fermi liquid state around $B_{mathrm{c}}$ forms through a very little change in c-f hybridization. This result is in sharp contrast to Ce- and Yb-based Kramers Kondo lattices which show significantly larger volume strains due to the high sensitivity of the Kondo temperature to hydrostatic pressure.
Inelastic neutron scattering experiments on poly crystalline sample of heavy-fermion compound YbCo$_2$Zn$_{20}$ were carried out in order to obtain microscopic insights on the ground state and its magnetic field response. At zero field at 300 mK, ine
Superconductivity in PrIr$_{2}$Zn$_{20}$ appears at $T_{rm c} = 0.05$ K in the presence of an antiferroquadrupolar order below $T_{rm Q} = 0.11$ K. We have studied pressure dependences of $T_{rm c}$, $T_{rm Q}$, and non-Fermi liquid behaviors in the
We present the electrical resistivity data under application of pressures up to $sim$ 26 GPa and down to 50 mK temperatures on YbFe$_2$Zn$_{20}$. We find a pressure induced magnetic phase transition with an onset at $p_c$=18.2$pm$0.8 GPa. At ambient
Magnetization, resistivity and specific heat measurements were performed on the solution-grown, single crystals of six GdT$_2$Zn$_{20}$ (T = Fe, Ru, Os, Co, Rh and Ir) compounds, as well as their Y analogues. For the Gd compounds, the Fe column membe
The hallmark of nematic order in iron-based superconductors is a resistivity anisotropy but it is unclear to which extent quasiparticle dispersions, lifetimes and coherence contribute. While the lifted degeneracy of the Fe $d_{xz}$ and $d_{yz}$ dispe