arXiv Analytics

Sign in

arXiv:2202.08610 [cond-mat.mes-hall]AbstractReferencesReviewsResources

Understanding the three-dimensional quantum Hall effect in generic multi-Weyl semimetals

Feng Xiong, Carsten Honerkamp, Dante M. Kennes, Tanay Nag

Published 2022-02-17Version 1

The quantum Hall effect in three-dimensional Weyl semimetal (WSM) receives significant attention for the emergence of the Fermi loop where the underlying two-dimensional Hall conductivity, namely, sheet Hall conductivity, shows quantized plateaus. Considering the tilted lattice models for multi Weyl semimetals (mWSMs), we systematically study the Landau levels (LLs) and magneto-Hall conductivity in the presence of parallel and perpendicular (with respect to the Weyl node's separation) magnetic field, i.e., $\mathbf{ B}\parallel z$ and $\mathbf{B}\parallel x$, to explore the impact of tilting and non-linearity in the dispersion. We make use of two (single) node low-energy models to qualitatively explain the emergence of mid-gap chiral (linear crossing of chiral) LLs on the lattice for $\mathbf{ B}\parallel z$ ($\mathbf{ B}\parallel x$). Remarkably, we find that the sheet Hall conductivity becomes quantized for $\mathbf{ B}\parallel z$ even when two Weyl nodes project onto a single Fermi point in two opposite surfaces, forming a Fermi loop with $k_z$ as the good quantum number. On the other hand, the Fermi loop, connecting two distinct Fermi points in two opposite surfaces, with $k_x$ being the good quantum number, causes the quantization in sheet Hall conductivity for $\mathbf{ B}\parallel x$. The quantization is almost lost (perfectly remained) in the type-II phase for $\mathbf{ B}\parallel x$ ($\mathbf{ B}\parallel z$). Interestingly, the jump profiles between the adjacent quantized plateaus change with the topological charge for both of the above cases. The momentum-integrated three-dimensional Hall conductivity is not quantized; however, it bears the signature of chiral LLs as resulting in the linear dependence on $\mu$ for small $\mu$. The linear zone (its slope) reduces (increases) as the tilt (topological charge) of the underlying WSM increases.

Related articles: Most relevant | Search more
arXiv:2309.05990 [cond-mat.mes-hall] (Published 2023-09-12)
Three-Dimensional Quantum Hall Effect in Topological Amorphous Metals
arXiv:2002.01315 [cond-mat.mes-hall] (Published 2020-02-04)
Disorder-induced coupling of Weyl nodes in WTe$_2$
arXiv:2107.04469 [cond-mat.mes-hall] (Published 2021-07-09)
Chirality flip of Weyl nodes and its manifestation in strained MoTe$_2$