Precursor to Quantum Criticality in Ce-Au-Al Quasicrystal Approximants

TL;DR

This study investigates Ce-Au-Al quasicrystal approximants, revealing signs of quantum criticality through susceptibility and specific heat measurements, with results consistent with Kramers doublet splitting and low-temperature magnetic behavior.

Contribution

It provides the first detailed low-temperature magnetic and thermodynamic analysis of Ce-Au-Al approximants, demonstrating quantum critical signatures similar to quasicrystals.

Findings

Susceptibility diverges as 1/T at low temperatures.

Magnetic field dependence resembles quantum critical systems.

Low-temperature specific heat shows Schottky anomaly from Ce$^{3+}$ splitting.

Abstract

Rare-earth element containing aperiodic quasicrystals and their related periodic approximant crystals can exhibit non-trivial physical properties at low temperatures. Here, we investigate the 1/1 and 2/1 approximant crystal phases of the Ce-Au-Al system by studying the ac-susceptibility and specific heat at low temperatures and in magnetic fields up to 12 T. We find that these systems display signs of quantum criticality similar to the observations in other claimed quantum critical systems, including the related Yb-Au-Al quasicrystal. In particular, the ac-susceptibility at low temperatures shows a diverging behavior $\chi \propto 1/T$ as the temperature decreases as well as cutoff-behavior in magnetic field. Notably, the field dependence of $\chi$ closely resembles that of quantum critical systems. However, the ac-susceptibility both in zero and nonzero magnetic fields can be understood from the splitting of a ground state Kramers doublet of Ce$^{3+}$. The high-temperature Curie-Weiss fit yields an effective magnetic moment of approximately 2.54$\mu_{\mathrm{B}}$ per Ce for both approximant systems, which is reduced to $\sim$2.0$\mu_{\mathrm{B}}$ at temperatures below 10 K. The low-temperature specific heat is dominated by the Schottky anomaly originating from the splitting of the Ce$^{3+}$ Kramers doublet, resulting in an entropy of $R\ln 2$ at around 10 K.