Abstract

We report the anomalous Hall effect (AHE) and the anomalous Nernst effect (ANE) data for the noncollinear Weyl semimetal CeAlSi. The anomalous Hall conductivity (${\ensuremath{\sigma}}_{ij}^{A}$) was measured for two different orientations of the magnetic field ($B$), namely ${\ensuremath{\sigma}}_{yz}^{A}$ for $B||a$ and ${\ensuremath{\sigma}}_{xy}^{A}$ for $B||c$, where $a$ and $c$ denote the crystallographic axes. We find that ${\ensuremath{\sigma}}_{xy}^{A}$ and ${\ensuremath{\sigma}}_{yz}^{A}$ are of opposite sign and both are large below the Curie temperature (${T}_{\mathrm{C}}$). In the paramagnetic phase, ${\ensuremath{\sigma}}_{xy}^{A}$ rises even more and goes through a maximum at $T\ensuremath{\approx}170\phantom{\rule{0.28em}{0ex}}\mathrm{K}$, whereas the absolute value of ${\ensuremath{\sigma}}_{yz}^{A}$ decreases with increasing temperature. The origin of the sign difference between ${\ensuremath{\sigma}}_{xy}^{A}$ and ${\ensuremath{\sigma}}_{yz}^{A}$ was attributed to the reconstruction of the band structure under the variation of the spin orientation. Further, in a system where humps in the AHE are present and scalar spin chirality is zero, we show that the $\mathbf{k}$-space topology plays an important role to determine the transport properties at both low and high temperatures. We also observed the anomalous contribution in the Nernst conductivity (${\ensuremath{\alpha}}_{xy}^{A}$) measured for $B||c$. ${\ensuremath{\alpha}}_{xy}^{A}/T$ turns out to be sizeable in the magnetic phase and above ${T}_{\mathrm{C}}$ slowly decreases with temperature. We were able to recreate the temperature dependencies of ${\ensuremath{\sigma}}_{xy}^{A}$ and ${\ensuremath{\alpha}}_{xy}^{A}/T$ in the paramagnetic phase using a single band toy model assuming a nonzero Berry curvature in the vicinity of the Weyl node. A decisive factor appears to be a small energy distance between the Fermi level and a Weyl point.

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