CeAu₂Bi crystallizes in P63/mmc, orders antiferromagnetically at 3.1 K with localized f-electrons, and hosts symmetry-protected crossings at kz=π.
CeAu$_{2}$Bi: a new nonsymmorphic antiferromagnetic compound
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abstract
Here we report the structural and electronic properties of CeAu$_{2}$Bi, a new heavy-fermion compound crystallizing in a nonsymmorphic hexagonal structure ($P63/mmc$). The Ce$^{3+}$ ions form a triangular lattice which orders antiferromagnetically below $T_{N} = 3.1$~K with a magnetic hard axis along the c-axis. Under applied pressure, $T_{N}$ increases linearly at a rate of $0.07$~K/kbar, indicating that the Ce $f$-electrons are fairly localized. In fact, heat capacity measurements provide an estimate of 150(10) mJ/mol.K$^{2}$ for the Sommerfeld coefficient. The crystal-field scheme obtained from our thermodynamic data points to a ground state with dominantly $|j_{z}=\pm1/2\rangle$ character, which commonly occurs in systems with a hard c-axis. Finally, electronic band structure calculations and symmetry analysis in $k$-space reveal that CeAu$_{2}$Bi hosts symmetry-protected crossings at $k_{z} = \pi$ in the paramagnetic state
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cond-mat.str-el 1years
2019 1verdicts
UNVERDICTED 1representative citing papers
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CeAu$_{2}$Bi: a new nonsymmorphic antiferromagnetic compound
CeAu₂Bi crystallizes in P63/mmc, orders antiferromagnetically at 3.1 K with localized f-electrons, and hosts symmetry-protected crossings at kz=π.