Anomalous Hall effects beyond Berry magnetic fields in a Weyl metal phase

Applying time-varying magnetic fields to Weyl metals, a pair of Weyl points becomes oscillating. This oscillating monopole and antimonopole pair gives rise to ac Berry magnetic fields, responsible for the emergence of Berry electric fields, which have not been discussed before at least in the context of Weyl metals. Introducing this information into Boltzmann transport theory, we find anomalous Hall effects beyond Berry magnetic fields as a fingerprint of Berry electric fields.

Figure 1

Direction of the anomalous Hall currents driven by the Berry electric field for the case of ${\mathit{B}}_0\left|\right|\mathit{E}\perp \dot{\mathit{c}}$.

Figure 2

$x$ vs $F_1\left(x\right)$.

Figure 3

Direction of the anomalous Hall current driven by the Berry electric field for the case of ${\mathit{B}}_0\perp \mathit{E}$ and ${\mathit{B}}_0\left|\right|\dot{\mathit{c}}$.

Figure 4

$x$ vs $F_2\left(x\right)$.

Figure 5

Direction of the anomalous Hall current driven by the Berry electric field for the case of ${\mathit{B}}_0\perp \mathit{E}, \mathit{E}\perp \dot{\mathit{c}}$, and ${\mathit{B}}_0\perp \dot{\mathit{c}}$.

Figure 6

$x$ vs $F_3\left(x\right)$.

Figure 7

$x$ vs $|F_1\left(x\right)|$ (red), $|F_2\left(x\right)|$ (blue), and $|F_3\left(x\right)|$ (black).