Related Experiment Video
Updated: Mar 17, 2026

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
Published on: June 28, 2018
Are the surface Fermi arcs in Dirac semimetals topologically protected?
Mehdi Kargarian1, Mohit Randeria1, Yuan-Ming Lu2
1Department of Physics, The Ohio State University, Columbus, OH 43210.
Surface states in Dirac semimetals (DSMs) are generally not topologically protected, unlike in Weyl semimetals. Experiments can test predictions for DSM surface state doping dependence.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Topological Materials
Background:
- Recent experiments explore anomalous surface states in Dirac semimetals (DSMs) like Na3Bi and Cd3As2.
- Understanding the topological protection of these surface states is crucial for their applications.
Purpose of the Study:
- To investigate the topological protection of gapless surface states in Dirac semimetals.
- To contrast the surface state properties of DSMs with those of Weyl semimetals.
Main Methods:
- Utilized a minimal four-band model with Dirac nodes.
- Performed K-theory analysis for the space groups of Na3Bi and Cd3As2.
- Investigated surface Brillouin zone properties.
Main Results:
- Gapless surface states in DSMs are not generally topologically protected, except on specific time-reversal-invariant planes.
- Surface states are protected near specific points in the surface Brillouin zone.
- Fermi arcs in DSMs generically deform into Fermi pockets, merging with bulk Dirac Fermi surface projections.
Conclusions:
- The topological protection of DSM surface states differs significantly from Weyl semimetals.
- Surface states exhibit doping-dependent behavior that can be experimentally verified.
- Findings provide insights into the fundamental properties of topological materials.
More Related Videos
09:06Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
04:51Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
Published on: July 8, 2021
Related Concept Videos
Fermi Level Dynamics
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Fermi Level
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Ferromagnetism
Equipotential Surfaces and Conductors
Semiconductors
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...