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Related Concept Videos

Motion Of A Charged Particle In A Magnetic Field01:22

Motion Of A Charged Particle In A Magnetic Field

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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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Magnetic Vector Potential01:15

Magnetic Vector Potential

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In electrostatics, the electric field can be written as the negative gradient of the potential. In magnetostatics, the zero divergence of the magnetic field ensures that the magnetic field can be expressed as the curl of a vector potential. This potential is known as the magnetic vector potential.
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
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Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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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.
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Gravitational Potential Energy for Extended Objects01:07

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Consider a system comprising several point masses. The coordinates of the center of mass for this system can be expressed as the summation of the product of each mass and its position vector divided by the total mass:
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Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

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In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
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Gravitation Between Spherically Symmetric Masses01:14

Gravitation Between Spherically Symmetric Masses

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The gravitational potential energy between two spherically symmetric bodies can be calculated from the masses and the distance between the bodies, assuming that the center of mass is concentrated at the respective centers of the bodies.
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Related Experiment Video

Updated: Apr 25, 2026

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Trapping massless Dirac particles in a rotating saddle.

Johan Nilsson1

  • 1Department of Physics, University of Gothenburg, 412 96 Gothenburg, Sweden.

Physical Review Letters
|August 29, 2014
PubMed
Summary

Rotating saddle potentials create localized states for electrons in graphene. These unique eigenstates exhibit extended lifetimes, even with system imperfections, offering insights into quantum particle behavior.

Area of Science:

  • Condensed Matter Physics
  • Quantum Mechanics

Background:

  • Rotating potentials can induce bounded motion for particles with parabolic dispersion.
  • Forces in rotating frames include potential, centrifugal, and Coriolis forces.

Purpose of the Study:

  • To investigate the behavior of massless Dirac particles in rotating saddle-shaped potentials.
  • To determine if such potentials lead to spatially localized eigenstates.

Main Methods:

  • Analysis of particle motion in two-dimensional rotating saddle-shaped potentials.
  • Application of the potential to massless Dirac particles, specifically electrons in graphene.

Main Results:

  • Spatially localized eigenstates are observed near the saddle center at specific energies.

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  • Nonoverlapping support in the oscillator basis for coexisting states.
  • Localized states demonstrate a substantial lifetime in the presence of imperfections.
  • Conclusions:

    • Rotating saddle potentials can effectively localize Dirac particles in specific energy ranges.
    • The observed localization and extended lifetime have implications for quantum systems and materials like graphene.