Related Experiment Video
Updated: Jan 2, 2026

06:43
Writing and Low-Temperature Characterization of Oxide Nanostructures
Published on: July 18, 2014
10.3K
Controlling a Van Hove singularity and Fermi surface topology at a complex oxide heterostructure interface
Ryo Mori1,2, Patrick B Marshall3, Kaveh Ahadi3
1Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA.
Nature Communications
|December 5, 2019
Summary
Researchers engineered electronic phases by tuning Fermi surface topology and Van Hove singularities (VHSs) at insulator interfaces. This method overcomes limitations of traditional doping, enabling new electronic phenomena.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Quantum Mechanics
Background:
- Saddle-point Van Hove singularities (VHSs) in density of states, coupled with Lifshitz transitions, foster diverse electronic phenomena like superconductivity and magnetism.
- Achieving these states is challenging as the Fermi level is often too distant from VHSs for conventional tuning methods.
Purpose of the Study:
- To demonstrate a novel method for accessing and engineering Van Hove singularities (VHSs) and Fermi surface topology.
- To explore the potential for realizing exotic electronic phases through interface engineering.
Main Methods:
- Investigated the interface between a Mott insulator and a band insulator.
- Utilized quantum confinement and correlation enhancement effects.
- Controlled electronic properties by adjusting layer thickness and orbital occupancy.
Main Results:
- Successfully realized saddle-point Van Hove singularities (VHSs) and altered Fermi surface topology at the insulator interface.
- Demonstrated tunability of these electronic properties via precise control over material parameters.
- Established a pathway to engineer electronic phases through interface modification.
Conclusions:
- Interface engineering between Mott and band insulators offers a viable route to tune Fermi surface topology and Van Hove singularities (VHSs).
- This approach facilitates the exploration of novel electronic phenomena, overcoming limitations of traditional tuning techniques.
Related Concept Videos
Biasing of Metal-Semiconductor Junctions
500
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
500
Metal-Semiconductor Junctions
838
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
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...
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...
838
Fermi Level Dynamics
606
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
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...
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...
606
Valence Bond Theory
10.9K
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
10.9K
Biasing of FET
632
Biasing a Junction Field Effect Transistor (JFET) is crucial for setting operational parameters and ensuring efficient functioning in electronic circuits. JFETs are characterized by using a single carrier type in N-channel or P-channel configurations, where the channel is surrounded by PN junctions. These junctions are central to the device's ability to control current flow.
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
632
MOSFET: Enhancement Mode
721
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
721

