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Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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. This...
Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Thomson's e/m Experiment01:19

Thomson's e/m Experiment

In a beam of charged particles created by a heated cathode, the particles move at different speeds. However, many applications need a beam with uniform particle speeds. An arrangement known as a velocity selector uses electric and magnetic fields to pick particles with a particular speed from the beam.
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The magnetic...
The de Broglie Wavelength02:32

The de Broglie Wavelength

In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
Motion Of A Charged Particle In A Magnetic Field01:22

Motion Of A Charged Particle In A Magnetic Field

A charged particle experiences a force when moving through a magnetic field. Consider the field to be uniform and the charged particle to move perpendicular to it. If the field is in a vacuum, the magnetic field is the dominant factor determining the motion. Since the magnetic force is perpendicular to the direction of motion, a charged particle follows a curved path. The particle continues to follow this curved path until it forms a complete circle. Another way to look at this is that the...

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Related Experiment Video

Updated: Jun 25, 2026

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
10:40

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

Published on: June 28, 2016

Dynamically induced Zeeman effect in massless QED.

Efrain J Ferrer1, Vivian de la Incera

  • 1Department of Physics, University of Texas at El Paso, El Paso, Texas 79968, USA.

Physical Review Letters
|March 5, 2009
PubMed
Summary
This summary is machine-generated.

In nonperturbative quantum electrodynamics, a magnetic field dynamically induces an anomalous magnetic moment in electrons. This effect causes Zeeman splitting in higher Landau levels, with implications for fundamental physics.

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Area of Science:

  • Quantum Electrodynamics (QED)
  • Condensed Matter Physics

Background:

  • Quantum electrodynamics describes interactions between charged particles and electromagnetic fields.
  • Landau levels describe the quantization of energy levels in a magnetic field.

Purpose of the Study:

  • To investigate the dynamic induction of an anomalous magnetic moment in nonperturbative massless QED.
  • To analyze the resulting Zeeman splitting in electron Landau levels.
  • To derive expressions for the Lande g factor and Bohr magneton.

Main Methods:

  • Nonperturbative theoretical calculations in massless QED.
  • Analysis of electron behavior in applied magnetic fields.
  • Derivation of quantum mechanical expressions.

Main Results:

  • An anomalous magnetic moment is dynamically induced by a magnetic field.
  • Zeeman splitting is observed in Landau levels above l=0.
  • Expressions for the nonperturbative Lande g factor and Bohr magneton were obtained.

Conclusions:

  • The study demonstrates a novel mechanism for magnetic moment induction in QED.
  • The findings have potential applications in understanding electron behavior in extreme magnetic fields.
  • This work provides a theoretical framework for experimental verification.