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Mass Analyzers: Common Types01:19

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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...
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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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Projection-type electron spectroscopy collimator analyzer for charged particles and x-ray detections.

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We created a compact device for analyzing charged particle energy and angle over a wide field of view. This electron-optical system achieves high angular resolution for surface emission measurements.

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Area of Science:

  • Physics
  • Materials Science
  • Analytical Chemistry

Background:

  • Characterizing charged particle emission requires precise angular and energy analysis.
  • Existing methods often lack wide acceptance angles or high resolution.

Purpose of the Study:

  • To develop a compact, high-resolution device for analyzing charged particle angular and energy distributions.
  • To enable efficient two-dimensional angular distribution measurements of emitted electrons and ions.

Main Methods:

  • Utilized an electrostatic lens with an axisymmetric aspherical mesh and electrodes to parallelize electron trajectories.
  • Incorporated planar grids or a collimator plate as an energy band-pass filter.
  • Employed microchannel plates and a fluorescent screen for direct projection of angular distribution.

Main Results:

  • Achieved a wide acceptance cone angle of nearly 1π steradian.
  • Demonstrated parallelization of electron trajectories for perpendicular entry into the energy filter.
  • Enabled direct projection of angular distribution onto a screen without a pinhole, ensuring high angular resolution.

Conclusions:

  • The developed device offers a simple yet significant electron-optical design for wide-range angular distribution analysis.
  • The analyzer is well-suited for two-dimensional angular distribution measurements of charged particles emitted from surfaces.
  • This compact instrument enhances the capability for detailed surface analysis in various scientific fields.