Related Experiment Video
Updated: Apr 5, 2026

07:17
Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
Published on: August 1, 2017
13.3K
Expansion-Driven Self-Magnetization of High-Energy-Density Plasmas
K V Lezhnin1, S R Totorica2,3, J Griff-McMahon1,2
1Princeton Plasma Physics Laboratory, 100 Stellarator Rd, Princeton, New Jersey 08540, USA.
Physical Review Letters
|April 3, 2026
Summary
High-energy plasma experiments show rapid self-magnetization above a critical laser intensity. This process, driven by expansion, generates strong magnetic fields that alter plasma heat transport, crucial for understanding fusion energy.
Area of Science:
- Plasma Physics
- High-Energy-Density (HED) Science
- Astrophysical Plasma Dynamics
Background:
- Self-magnetization is a key challenge in laboratory and astrophysical plasmas, influencing plasma transport and evolution.
- Previous high-energy-density experiments observed ion-scale magnetic filaments, but their origin is debated.
Purpose of the Study:
- To investigate the origin of plasma self-magnetization in 2D collisional particle-in-cell (PIC) simulations.
- To understand the role of anisotropy-driven instabilities in magnetic field generation.
- To explore the impact of self-generated magnetic fields on plasma transport properties.
Main Methods:
- Conducted 2D collisional particle-in-cell (PIC) simulations with a laser ray-tracing module.
- Utilized planar geometry to suppress Biermann magnetic fields and focus on anisotropy-driven instabilities.
- Varied laser intensity between 10^13 and 10^14 W/cm^2, considering collisional effects relevant to HED and inertial fusion.
Main Results:
- Identified a critical laser intensity threshold for rapid plasma self-magnetization.
- Observed an expansion-driven Weibel process generating magnetic fields.
- Achieved plasma beta (β) of 100 and Hall parameter (ω_ceτ_e) > 1 within picoseconds.
- Demonstrated that generated magnetic fields significantly modify plasma heat transport.
Conclusions:
- Plasma self-magnetization occurs rapidly via an expansion-driven Weibel process above a critical laser intensity.
- The generated magnetic fields are strong enough to alter plasma heat transport, impacting plasma dynamics.
- These findings are crucial for understanding magnetic field generation in HED and inertial fusion experiments.
Related Concept Videos
Potential Due to a Magnetized Object
885
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
The vector...
885
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
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
Energy In A Magnetic Field
3.0K
If a magnetic field is sustained, there must be a current in a closed circuit or loop, implying some energy has been spent in creating the field. If this energy is not dissipated via the circuit's resistance, it is stored in the field.
Take an ideal inductor with zero resistance. Although it's practically impossible, assume that the coil's resistance is so small that it is practically negligible. The loss of the field's energy to dissipate thermal energy (or heat) is thus...
Take an ideal inductor with zero resistance. Although it's practically impossible, assume that the coil's resistance is so small that it is practically negligible. The loss of the field's energy to dissipate thermal energy (or heat) is thus...
3.0K
Diamagnetism
3.4K
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....
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

