Related Experiment Video
Updated: May 30, 2026

13:05
Plasma-Assisted Molecular Beam Epitaxy Growth of Mg3N2 and Zn3N2 Thin Films
Published on: May 11, 2019
Li(Zn,Mn)As as a new generation ferromagnet based on a I-II-V semiconductor
1Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
Nature Communications
|August 11, 2011
Summary
Researchers synthesized bulk Li(Zn,Mn)As, a novel ferromagnetic material. This overcomes limitations of (Ga,Mn)As, enabling potential for new semiconductor devices.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Semiconductor Spintronics
Background:
- Traditional (Ga,Mn)As ferromagnets have limited solubility and cannot be electron-doped.
- Isovalent substitution in LiZnAs offers a theoretical route to decouple magnetism from carrier doping.
Purpose of the Study:
- To synthesize bulk Li(Zn,Mn)As materials.
- To investigate the magnetic properties and carrier types of these novel compounds.
- To explore potential applications in future electronic devices.
Main Methods:
- Solid-state synthesis of Li(1+y)(Zn(1-x)Mn(x))As bulk materials.
- Characterization of magnetic properties, including critical temperature (Tc).
- Analysis of carrier type and concentration.
Main Results:
- Successful synthesis of bulk Li(1+y)(Zn(1-x)Mn(x))As.
- Observation of ferromagnetism with Tc up to 50 K in Li-excess samples (y=0.05-0.2, x=0.02-0.15).
- Identification of p-type metallic carriers, attributed to excess Li substitution.
Conclusions:
- Isovalent substitution in LiZnAs provides a viable method for creating bulk ferromagnetic materials.
- The shared square lattice As layers across related Li-based compounds suggest potential for novel junction devices.
Related Concept Videos
Ferromagnetism
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
Semiconductors
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
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...
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...
Valence Bond Theory
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...
Types Of Superconductors
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
Metal-Semiconductor Junctions
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 semiconductor's...
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 semiconductor's...
Types of Semiconductors
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...

