Related Experiment Video
Updated: Aug 7, 2025

08:25
Chemical Vapor Deposition of an Organic Magnet, Vanadium Tetracyanoethylene
Published on: July 3, 2015
11.5K
Room-Temperature Magnetism in 2D MnGa4 -H Induced by Hydrogen Insertion
Nan Wei1, Liangcheng He1, Changwei Wu2,3
1College of Chemistry and Molecular Sciences, Wuhan University, Wuhan, 430072, P. R. China.
Advanced Materials (Deerfield Beach, Fla.)
|March 10, 2023
Summary
Researchers developed a new 2D room-temperature magnetic material, MnGa₄-H, using plasma-enhanced chemical vapor deposition. This breakthrough advances the field of 2D magnetic alloys for spintronic devices.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Nanotechnology
Background:
- 2D room-temperature magnetic materials are crucial for next-generation spintronic devices.
- The scarcity of such materials limits advancements in spintronics.
Purpose of the Study:
- To synthesize a novel 2D room-temperature magnetic material.
- To explore the potential of plasma-enhanced chemical vapor deposition (PECVD) for creating these materials.
- To investigate the magnetic properties and stability of the synthesized material.
Main Methods:
- Plasma-enhanced chemical vapor deposition (PECVD) was used to synthesize 2D MnGa₄-H single crystals.
- Hydrogen plasma was employed to introduce hydrogen atoms into the MnGa₄ lattice.
- Structural and magnetic properties were characterized.
Main Results:
- A high-quality, air-stable, and thermo-stable 2D MnGa₄-H single crystal was successfully synthesized with a thickness down to 2.2 nm.
- The material exhibits robust room-temperature ferrimagnetism with a high Curie temperature exceeding 620 K.
- Hydrogen insertion modulated lattice parameters and charge states, enabling magnetism without structural degradation.
Conclusions:
- The development of 2D MnGa₄-H enriches the family of 2D room-temperature magnetic materials.
- This material holds significant promise for the development of advanced spintronic devices.
- The PECVD approach offers a viable route for fabricating novel 2D magnetic alloys.
Related Concept Videos
Paramagnetism
2.6K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
2.6K
Ferromagnetism
2.4K
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...
2.4K
Diamagnetism
2.5K
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
2.5K
π Electron Effects on Chemical Shift: Overview
1.1K
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.1K
Magnetic Susceptibility and Permeability
1.3K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
1.3K
Atomic Nuclei: Nuclear Magnetic Moment
1.3K
All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
1.3K

