AI Article Synopsis

  • The study focuses on the chirality of massless fermions in Dirac semimetals, revealing its importance for understanding their behavior and potential applications.
  • It shows that circularly polarized light can create an isospin polarization, which labels the chirality of these carriers, in the Dirac semimetal CdAs.
  • The findings indicate a long scattering time and decay time for the isospin, suggesting that Dirac semimetals could have promising uses in future tech due to their robust and reversible properties.

Article Abstract

Chirality of massless fermions emerging in condensed matter is a key to understand their characteristic behavior as well as to exploit their functionality. However, the chiral nature of massless fermions in Dirac semimetals has remained elusive, due to equivalent occupation of carriers with the opposite chirality in thermal equilibrium. Here, we show that the isospin degree of freedom, which labels the chirality of massless carriers from a crystallographic point of view, can be injected by circularly polarized light. Terahertz Faraday rotation spectroscopy successfully detects the anomalous Hall conductivity by a light-induced isospin polarization in a three-dimensional Dirac semimetal, CdAs. Spectral analysis of the Hall conductivity reveals a long scattering time and a long decay time, which are characteristic of the isospin. The long-lived, robust, and reversible character of the isospin promises a potential application of Dirac semimetals in future information technology.

Download full-text PDF

Source
http://dx.doi.org/10.1021/acs.nanolett.3c03770DOI Listing

Publication Analysis

Top Keywords

anomalous hall
8
isospin degree
8
degree freedom
8
dirac semimetal
8
chirality massless
8
massless fermions
8
dirac semimetals
8
hall conductivity
8
isospin
5
hall transport
4

Similar Publications

Using a full-wave theory to analyze the light beam scattering at sharp interfaces, we reexamine the anomalous spin-orbit interaction (SOI) around the Fresnel coefficient (FC) singularities. We evaluate the spin-dependent beam shifts near the singularity for three typical optical interfaces, comparing our results with existing ones. Existing theories neglect the contribution of the wave vector component near the FC singularities, potentially leading to erroneous results.

View Article and Find Full Text PDF

Non-Hermitian Theory of Valley Excitons in Two-Dimensional Semiconductors.

Phys Rev Lett

December 2024

School of Physics and Electronics, Hunan University, Changsha 410082, China.

Electron-hole exchange interaction in two-dimensional transition metal dichalcogenides is extremely strong due to the dimension reduction, which promises valley-superposed excitonic states with linearly polarized optical emissions. However, strong circular polarization reflecting valley-polarized excitonic states is commonly observed in helicity-resolved optical experiments. Here, we present a non-Hermitian theory of valley excitons by incorporating optical pumping and intrinsic decay, which unveils an anomalous valley-polarized excitonic state with elliptically polarized optical emission.

View Article and Find Full Text PDF

For over a century, the Hall effect, a transverse effect under an out-of-plane magnetic field or magnetization, has been a cornerstone for magnetotransport studies and applications. Modern theoretical formulation based on the Berry curvature has revealed the potential that even an in-plane magnetic field can induce an anomalous Hall effect, but its experimental demonstration has remained difficult due to its potentially small magnitude and strict symmetry requirements. Here, we report observation of the in-plane anomalous Hall effect by measuring low-carrier density films of magnetic Weyl semimetal EuCd_{2}Sb_{2}.

View Article and Find Full Text PDF

Critical Nematic Phase with Pseudogaplike Behavior in Twisted Bilayers.

Phys Rev Lett

December 2024

School of Physics and Astronomy, University of Minnesota, Minneapolis, Minnesota 55455, USA.

The crystallographic restriction theorem constrains two-dimensional nematicity to display either Ising (Z_{2}) or three-state-Potts (Z_{3}) critical behaviors, both of which are dominated by amplitude fluctuations. Here, we use group theory and microscopic modeling to show that this constraint is circumvented in a 30°-twisted hexagonal bilayer due to its emergent quasicrystalline symmetries. We find a critical phase dominated by phase fluctuations of a Z_{6} nematic order parameter and bounded by two Berezinskii-Kosterlitz-Thouless (BKT) transitions, which displays only quasi-long-range nematic order.

View Article and Find Full Text PDF

Want AI Summaries of new PubMed Abstracts delivered to your In-box?

Enter search terms and have AI summaries delivered each week - change queries or unsubscribe any time!