Related Experiment Video
Updated: Mar 19, 2026

09:06
Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
8.7K
Ultrafast Magnetic Order Transition Driven by Excited-State Carrier Relaxation in Ferromagnetic Heterostructures.
Yuchong Kang1, Jian Yuan1, Shunwei Yao1
1School of Physics, Sun Yat-Sen University, Guangzhou 510275, China.
The Journal of Physical Chemistry Letters
|March 18, 2026
Summary
Researchers demonstrated ultrafast magnetic state switching in CrI3/CrBr3 heterostructures using photoexcited electrons. This discovery enables rapid, stable magnetic state generation for spintronic devices.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Spintronics
Background:
- All-optical control of magnetism is crucial for ultrafast spintronic devices.
- Generating transient magnetic states with long-term stability is a significant challenge.
Purpose of the Study:
- To propose and investigate the potential of photoexcited electron relaxation in type-II spin-antiparallel heterostructures for creating multiple stable magnetic states.
- To understand the dynamics of ultrafast magnetic phase transitions.
Main Methods:
- Photoinduced spin-dynamics simulations were performed on the CrI3/CrBr3 heterostructure.
- The influence of electron-phonon coupling (EPC) and spin-orbit coupling (SOC) on relaxation pathways and rates was analyzed.
Main Results:
- An ultrafast phase transition from antiferromagnetic (AFM) to ferrimagnetic (FiM) state was observed within 826 fs.
- The competition between EPC and SOC critically determines relaxation pathways and rates.
- Exciting electrons to higher-energy states accelerated the phase transition to 346 fs due to enhanced EPC and SOC.
Conclusions:
- The study advances the understanding of dynamic coupling between spin, charge, and lattice degrees of freedom in ultrafast magnetic order transitions.
- The findings pave the way for developing advanced nonvolatile memory and neuromorphic computing systems.
Related Concept Videos
Atomic Nuclei: Nuclear Relaxation Processes
1.4K
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
1.4K
Ferromagnetism
3.4K
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...
3.4K
Atomic Nuclei: Magnetic Resonance
1.4K
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
1.4K
Paramagnetism
3.2K
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...
3.2K
Colors and Magnetism
14.5K
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...
14.5K
Carrier Generation and Recombination
1.5K
Carrier generation is the process by which electron-hole pairs (EHPs) are created within the semiconductor. In direct-bandgap semiconductors, such as gallium arsenide (GaAs), this occurs efficiently when energy absorption prompts valence electrons to leap into the conduction band, leaving behind holes.
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
1.5K

