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Related Concept Videos

Atomic Emission Spectroscopy: Lab01:29

Atomic Emission Spectroscopy: Lab

AES is a powerful analytical technique, especially effective when used with plasma sources, producing abundant spectra in characteristic emission lines. The Inductively Coupled Plasma (ICP), in particular, yields superior quantitative analytical data due to its high stability, low noise, low background, and minimal interferences under optimal experimental conditions. However, newer air-operated microwave sources are emerging as promising alternatives that could be more cost-effective than...
Inductively Coupled Plasma–Mass Spectrometry (ICP–MS): Overview01:19

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In inductively coupled plasma–mass spectrometry (ICP–MS), an inductively coupled plasma (ICP) torch is used as an atomizer and ionizer. Solid samples are dissolved and volatilized before being introduced into the high-temperature argon plasma, while solution samples are nebulized and passed through the high-temperature argon plasma. Plasma dissociates the analytes and ionizes their component atoms to form a mixture of positive ions and molecular species. The positive ions are then passed on to...
Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation01:26

Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation

Inductively coupled plasma (ICP) is the common plasma source used in atomic emission spectroscopy (AES), a technique that detects and analyzes various elements in a sample. This method is often called inductively coupled plasma atomic emission spectroscopy (ICP-AES).
There are three main types of inductively coupled plasma atomic emission spectroscopy  (ICP-AES) instruments: sequential, simultaneous multichannel, and Fourier transform instruments, with the latter being less commonly used.
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.

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Updated: Jun 5, 2026

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
07:17

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry

Published on: August 1, 2017

Note: Zeeman splitting measurements in a high-temperature plasma.

R P Golingo1, U Shumlak, D J Den Hartog

  • 1Aerospace and Energetics Research Program, University of Washington, Seattle, Washington 98195-2250, USA. golingo@aa.washington.edu

The Review of Scientific Instruments
|January 5, 2011
PubMed
Summary

New methods enable accurate magnetic field measurement in high-temperature plasmas using the Zeeman effect. This technique is crucial for understanding plasma behavior in devices like the ZaP Z-pinch.

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Area of Science:

  • Plasma physics
  • Spectroscopy
  • Magnetohydrodynamics

Background:

  • The Zeeman effect is a standard diagnostic for magnetic fields in low-temperature plasmas.
  • Traditional Zeeman spectroscopy is challenging in high-temperature plasmas due to spectral broadening.

Purpose of the Study:

  • To develop and demonstrate a new method for simultaneous measurement of Doppler-broadened, circularly polarized Zeeman spectra.
  • To accurately measure magnetic fields in high-temperature plasmas, specifically within the ZaP Z-pinch device.

Main Methods:

  • Utilized new instrumentation for simultaneous recording of left and right circularly polarized Zeeman spectra.
  • Measured spectra emitted parallel to the magnetic field from carbon impurities.
  • Collected spectral data along multiple chords across the plasma cross-section.

Main Results:

  • Successfully measured simultaneous Doppler-broadened Zeeman spectra in a high-temperature plasma.
  • Determined the location of the Z-pinch current axis.
  • Provided lower-bound estimates of local magnetic fields at radial locations.

Conclusions:

  • The developed technique overcomes limitations of traditional Zeeman spectroscopy in high-temperature environments.
  • This method allows for precise magnetic field mapping within Z-pinch plasmas.
  • Enables better understanding of plasma dynamics and magnetic field configurations.