Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Mass Analyzers: Common Types01:19

Mass Analyzers: Common Types

The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
Mass Analyzers: Overview01:13

Mass Analyzers: Overview

The mass analyzer is a crucial component of the mass spectrometer. In the ionization chamber, the vaporized sample is bombarded with a high-energy electron beam to generate a radical cation and further fragment into neutral molecules, radicals, and cations. A series of negatively charged accelerator plates accelerate the cations into the mass analyzer. The mass analyzer separates ions according to their mass-to-charge (m/z) ratios and then directs them to the detector. The common types of mass...
Atomic Emission Spectroscopy: Instrumentation01:22

Atomic Emission Spectroscopy: Instrumentation

The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers.  Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
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...

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Carrier-Envelope Phase-Dependent Strong-Field Excitation.

Physical review letters·2022
Same author

Relativistic Nondipole Effects in Strong-Field Atomic Ionization at Moderate Intensities.

Physical review letters·2019
Same author

Author Correction: Attosecond angular streaking and tunnelling time in atomic hydrogen.

Nature·2019
Same author

Attosecond angular streaking and tunnelling time in atomic hydrogen.

Nature·2019
Same author

Plasma plumes produced by laser ablation of Al with single and double pulse schemes.

Optics letters·2018
Same author

Laser-Based Metastable Krypton Generation.

Physical review letters·2018

Related Experiment Video

Updated: Jul 13, 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

Absolute metastable atom-atom collision cross section measurements using a magneto-optical trap.

K J Matherson1, R D Glover, D E Laban

  • 1Centre for Quantum Dynamics, Griffith University, Nathan QLD 4111, Australia.

The Review of Scientific Instruments
|August 4, 2007
PubMed
Summary

We developed a new method to measure collision cross sections for metastable neon atoms. This technique was used to determine the cross section for neon atoms colliding with argon, yielding 556+/-26 A(2).

More Related Videos

Optical Trap Loading of Dielectric Microparticles In Air
08:57

Optical Trap Loading of Dielectric Microparticles In Air

Published on: February 5, 2017

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps
11:45

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps

Published on: August 17, 2017

Related Experiment Videos

Last Updated: Jul 13, 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

Optical Trap Loading of Dielectric Microparticles In Air
08:57

Optical Trap Loading of Dielectric Microparticles In Air

Published on: February 5, 2017

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps
11:45

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps

Published on: August 17, 2017

Area of Science:

  • Atomic physics
  • Quantum mechanics
  • Collision cross sections

Background:

  • Metastable atoms are crucial in various physical and chemical processes.
  • Measuring collision cross sections provides fundamental insights into atomic interactions.

Purpose of the Study:

  • To introduce a novel technique for measuring absolute total collision cross sections of metastable neon atoms.
  • To perform the first measurement of this kind using trapped metastable neon atoms.

Main Methods:

  • Utilizing the decay rate of trapped metastable neon atoms.
  • Observing collisions between trapped (3)P(2) metastable neon atoms and room temperature ground state argon atoms.

Main Results:

  • Successfully measured the absolute total collision cross section for metastable neon-argon interactions.
  • Obtained a cross section value of 556+/-26 A(2).

Conclusions:

  • The new technique provides a reliable method for determining collision cross sections of metastable atoms.
  • The measured cross section offers valuable data for understanding neon-argon interactions at the atomic level.