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Electromagnetic Waves in Matter01:30

Electromagnetic Waves in Matter

Electromagnetic waves can travel in the vacuum as well as in matter. For example light, which is an electromagnetic wave, can travel through air, water, or glass.
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the medium, μ.
Furthermore, the...
π Electron Effects on Chemical Shift: Overview01:27

π Electron Effects on Chemical Shift: Overview

An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0, resulting in...
Fermi Level Dynamics01:12

Fermi Level Dynamics

The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron Orbital Model01:18

Electron Orbital Model

Orbitals are the areas outside of the atomic nucleus where electrons are most likely to reside. They are characterized by different energy levels, shapes, and three-dimensional orientations. The location of electrons is described most generally by a shell or principal energy level, then by a subshell within each shell, and finally, by individual orbitals found within the subshells.The first shell is closest to the nucleus, and it has only one subshell with a single spherical orbital called the...
Electron Configuration of Multielectron Atoms03:26

Electron Configuration of Multielectron Atoms

The alkali metal sodium (atomic number 11) has one more electron than the neon atom. This electron must go into the lowest-energy subshell available, the 3s orbital, giving a 1s22s22p63s1 configuration. The electrons occupying the outermost shell orbital(s) (highest value of n) are called valence electrons, and those occupying the inner shell orbitals are called core electrons. Since the core electron shells correspond to noble gas electron configurations, we can abbreviate electron...
Cryo-electron Microscopy01:28

Cryo-electron Microscopy

Conventional electron microscopy (EM) involves dehydration, fixation, and staining of biological samples, which distorts the native state of biological molecules and results in several artifacts. Also, the high-energy electron beam damages the sample and makes it difficult to obtain high-resolution images. These issues can be addressed using cryo-EM, which uses frozen samples and gentler electron beams. The technique was developed by Jacques Dubochet, Joachim Frank, and Richard Henderson, for...

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Related Experiment Video

Updated: Jun 23, 2026

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

Coherent electron cooling.

Vladimir N Litvinenko1, Yaroslav S Derbenev

  • 1Brookhaven National Laboratory, Upton, Long Island, New York, USA. vl@bnl.gov

Physical Review Letters
|April 28, 2009
PubMed
Summary
This summary is machine-generated.

Cooling high-energy particle beams is difficult. A new method using a high-gain free-electron laser (FEL) offers a solution for coherent electron cooling, potentially improving collider luminosity.

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Related Experiment Videos

Last Updated: Jun 23, 2026

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

Angle-resolved Photoemission Spectroscopy At Ultra-low Temperatures
08:53

Angle-resolved Photoemission Spectroscopy At Ultra-low Temperatures

Published on: October 9, 2012

Area of Science:

  • Accelerator Physics
  • Beam Cooling Techniques
  • High-Energy Particle Colliders

Background:

  • Cooling intense high-energy hadron beams presents a significant challenge in modern accelerator physics.
  • Synchrotron radiation is insufficient for cooling beams in accelerators like the Large Hadron Collider (LHC).
  • Existing cooling methods are inadequate for LHC-class proton beams.

Purpose of the Study:

  • To introduce a novel method for cooling high-energy particle beams.
  • To address the limitations of traditional cooling techniques for hadron colliders.
  • To propose a viable solution for achieving higher luminosities in particle colliders.

Main Methods:

  • Development of a novel coherent electron cooling technique.
  • Utilizing a high-gain free-electron laser (FEL) as the core component.
  • Theoretical analysis of the proposed cooling mechanism.

Main Results:

  • The proposed coherent electron cooling method is based on a high-gain free-electron laser.
  • This technique offers a potential solution for cooling intense high-energy hadron beams.
  • The method is expected to be effective where traditional methods fail.

Conclusions:

  • Coherent electron cooling using a high-gain FEL is a promising new technique.
  • This method could be crucial for enhancing luminosity in future hadron and electron-hadron colliders.
  • The proposed technique addresses a critical challenge in accelerator physics.