Emergent and robust ferromagnetic-insulating state in highly strained ferroelastic LaCoO3 thin films
Dong Li1, Hongguang Wang2, Kaifeng Li1
1College of Physics, MIIT Key Laboratory of Aerospace Information Materials and Physics, State Key Laboratory of Mechanics and Control for Aerospace Structures, Nanjing University of Aeronautics and Astronautics, 211106, Nanjing, China.
Nature Communications
|June 19, 2023
Summary
Tensile strain in LaCoO3 films induces ferromagnetism by creating ordered oxygen vacancies and altering cobalt ion states. This discovery offers insights into emergent ferromagnetic-insulating states for spintronic applications.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Solid State Chemistry
Background:
- Transition metal oxides exhibit tunable properties for spintronics.
- Ferroelastic lanthanum cobalt oxide (LaCoO3) is typically paramagnetic in bulk.
- Unexpected ferromagnetism in strained LaCoO3 films lacks a clear mechanistic explanation.
Purpose of the Study:
- To elucidate the origin of ferromagnetism in tensile-strained LaCoO3 films.
- To investigate the roles of oxygen vacancies and structural changes.
- To understand the electronic state modifications leading to ferromagnetism.
Main Methods:
- Experimental characterization of strained LaCoO3 films.
- Analysis of oxygen vacancy ordering and CoO6 octahedral rotations.
- Density functional theory (DFT) calculations.
Main Results:
- Simultaneous observation of ordered oxygen vacancies and suppressed octahedral rotations.
- DFT calculations reveal modified Co 3d-O 2p hybridization.
- Weakened crystal-field splitting and facilitated high-spin state of Co ions.
Conclusions:
- Strain-induced structural and electronic changes drive ferromagnetism in LaCoO3 films.
- An emergent ferromagnetic-insulating state arises from ordered oxygen vacancies and high-spin Co ions.
- Findings suggest potential for low-power spintronic devices.
More Related Videos
Related Concept Videos
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
Colors and Magnetism
12.0K
Color in Coordination Complexes
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
12.0K
Elastic Strain Energy for Shearing Stresses
231
As discussed in previous lessons, strain energy in a material is the energy stored when it is elastically deformed, a concept crucial in materials science and mechanical engineering. This energy results from the internal work done against the cohesive forces within the material. When a material undergoes shearing stress and corresponding shearing strain, the strain energy density, which is the energy stored per unit volume, is calculated. Within the elastic limit, where the stress is...
231
Theory of Metallic Conduction
1.4K
The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
1.4K
Diamagnetism
2.4K
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....
2.4K
Magnetic Susceptibility and Permeability
1.2K
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...
1.2K


