Related Experiment Video
Updated: Oct 4, 2025

08:01
Spectral and Angle-Resolved Magneto-Optical Characterization of Photonic Nanostructures
Published on: November 21, 2019
7.3K
Polarized phonons carry angular momentum in ultrafast demagnetization
S R Tauchert1,2, M Volkov1,2, D Ehberger2
1Universität Konstanz, Fachbereich Physik, Konstanz, Germany.
Nature
|February 3, 2022
Summary
Ultrafast laser pulses rapidly demagnetize nickel films by exciting unique, long-lasting, anisotropic phonons. These circularly polarized phonons absorb the spin system's angular momentum, explaining rapid magnetic order loss.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Ultrafast Phenomena
Background:
- Magnetic phenomena are crucial for technology, but rapid control of magnetic order is challenging.
- Ultrashort laser pulses can demagnetize materials like nickel on femtosecond timescales, opening avenues for ultrafast spintronics.
Purpose of the Study:
- To investigate the mechanism behind ultrafast demagnetization in nickel films.
- To identify the fate of angular momentum during rapid magnetic order loss.
Main Methods:
- Utilized ultrafast electron diffraction to probe atomic dynamics.
- Analyzed the temporal evolution of material properties after laser excitation.
Main Results:
- Observed an instantaneous, long-lasting population of anisotropic high-frequency phonons (150-750 fs) in nickel.
- Determined that phonon anisotropy plane is perpendicular to initial magnetization with 2 pm oscillation amplitude.
- Proposed circularly polarized phonons absorb angular momentum from the spin system.
Conclusions:
- Demagnetization time is linked to atomic acceleration via phonon excitation.
- Provides an atomistic explanation for the Einstein-de Haas effect.
- Highlights the significance of polarized phonons in non-equilibrium dynamics and phase transitions.
Related Concept Videos
Atomic Nuclei: Nuclear Relaxation Processes
754
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.
754
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
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
Atomic Nuclei: Magnetic Resonance
793
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...
793
Potential Due to a Polarized Object
496
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
496
Magnetic Moment of an Electron
1.9K
Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...
1.9K

