Samarium hexaboride is a trivial surface conductor
P Hlawenka1,2, K Siemensmeyer1, E Weschke1
1Helmholtz-Zentrum Berlin für Materialien und Energie, Elektronenspeicherring BESSY II, Albert-Einstein-Straße 15, 12489, Berlin, Germany.
Nature Communications
|February 8, 2018
Summary
Samarium hexaboride (SmB6) shows surface conductivity, but its surface states are topologically trivial, not matching predictions for topological Kondo insulators. A surface shift in its electronic resonance explains the observed conductivity.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Quantum Materials
Background:
- Samarium hexaboride (SmB6) is a candidate topological Kondo insulator.
- This material exhibits strong electron correlations and hybridization between localized and itinerant states.
- Surface-only conductivity at low temperatures suggests unique electronic properties.
Purpose of the Study:
- To investigate the topological nature of surface states in SmB6.
- To reconcile the observed surface conductivity with theoretical predictions.
- To understand the electronic structure of SmB6 at the (100) surface.
Main Methods:
- Low-temperature experimental measurements.
- Surface-sensitive electronic structure probes.
- Theoretical modeling of electronic states.
Main Results:
- The surface states at the (100) surface of SmB6 were found to be topologically trivial.
- A Rashba splitting was observed in a specific electronic state.
- A surface shift of the many-body resonance was proposed to explain the prominent observed state and surface conductivity.
Conclusions:
- The findings challenge the classification of SmB6 as a topological Kondo insulator.
- The observed surface conductivity can be explained by a surface-induced shift in the electronic resonance.
- A definitive link between topological insulators and Kondo insulators in SmB6 remains unconfirmed.
Related Concept Videos
Equipotential Surfaces and Conductors
4.5K
For a conductor in which all charges are at rest, the conductor's surface is equipotential. The electric field is always perpendicular to equipotential surfaces. Therefore, in a conductor with static charges, the electric field just outside the conductor is always perpendicular to the conductor's surface. Any tangential component of the electric field will cause charges to move inside the conductor, which will violate the electrostatic nature of the system. In an electrostatic...
4.5K
Electric Field at the Surface of a Conductor
5.4K
Consider a conductor in electrostatic equilibrium. The net electric field inside a conductor vanishes, and extra charges on the conductor reside on its outer surface, regardless of where they originate.
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...
5.4K
Conductors and Insulators
10.9K
Some materials may easily let electrical charges pass through them, while others obstruct their flow. The former are called conductors and the latter insulators. The atomic structures of materials determine whether they are conductors or insulators of electricity.
Most metals are conductors. Their atomic configuration is such that one or more electron(s) are loosely bound to the nucleus in each atom. Thus, a sea of mobile electrons are available in them, known as free electrons. Their easy...
Most metals are conductors. Their atomic configuration is such that one or more electron(s) are loosely bound to the nucleus in each atom. Thus, a sea of mobile electrons are available in them, known as free electrons. Their easy...
10.9K
Charge on a Conductor
5.4K
An interesting property of a conductor in static equilibrium is that extra charges on the conductor end up on its outer surface, regardless of where they originate. Consider a hollow metallic conductor with a uniform surface charge density. Since the conductor itself is in electrostatic equilibrium, there should not be any electric field inside the conductor. Now, assume a Gaussian surface enclosing the hollow portion. Applying Gauss's law, the inner surface of the hollow conductor will not...
5.4K
Electric Field Inside a Conductor
7.5K
When a conductor is placed in an external electric field, the free charges in the conductor redistribute and very quickly reach electrostatic equilibrium. The resulting charge distribution and its electric field have many interesting properties, which can be investigated with the help of Gauss's law.
Suppose a piece of metal is placed near a positive charge. The free electrons in the metal are attracted to the external positive charge and migrate freely toward that region. This region then...
Suppose a piece of metal is placed near a positive charge. The free electrons in the metal are attracted to the external positive charge and migrate freely toward that region. This region then...
7.5K
Charging Conductors By Induction
9.3K
The Earth is a good conductor of electricity, and it is so big that it can be considered an infinite source or sink of charges. It can easily exchange charges with any matter.
Generally, conductors like metals do not allow any excess charge to be present on them. Any excess charge added to metals easily flows away, for example, when a metal is placed on the Earth. This process is called earthing.
However, conductors can be charged by a process called induction. For example, consider charging a...
Generally, conductors like metals do not allow any excess charge to be present on them. Any excess charge added to metals easily flows away, for example, when a metal is placed on the Earth. This process is called earthing.
However, conductors can be charged by a process called induction. For example, consider charging a...
9.3K


