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Related Concept Videos

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.
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: 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...
Atomic Emission Spectroscopy: Overview01:20

Atomic Emission Spectroscopy: Overview

Atomic emission spectroscopy (AES) is an analytical technique used to determine the elemental composition of a sample by analyzing the light emitted from excited atoms. In AES, atoms in a sample are excited to higher energy levels by thermal energy from high-temperature sources, such as plasma, arcs, or sparks. When these excited atoms return to lower energy states, they emit light at specific wavelengths characteristic of each element. The resulting atomic emission spectrum, which consists of...
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

An atomic absorption spectrophotometer (AAS) comprises several components: a radiation source, an atomizer, a monochromator, and a detector. The radiation source can be a hollow-cathode lamp (HCL) or an electrodeless-discharge lamp (EDL), both of which provide a narrow emission line of the required wavelength. However, some instruments use continuum sources and high-resolution monochromators to achieve a narrow range of radiation.
The atomizer used in AAS can be either a flame atomizer or an...
Tandem Mass Spectrometry01:21

Tandem Mass Spectrometry

Tandem mass spectrometry is a technique that uses multiple mass analyzers in series to obtain a higher selectivity and reduce chemical noise during analyte detection. Instruments with multiple analyzers separated by an interaction cell enable secondary fragmentation and selected study of the fragment ions.Secondary fragmentations occur in the interaction cell and can be induced by various factors. Fragmentation induced by collision with inert gases, such as N2, Ar, He, etc., is called...

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Related Experiment Video

Updated: May 25, 2026

Quantitative Atomic-Site Analysis of Functional Dopants/Point Defects in Crystalline Materials by Electron-Channeling-Enhanced Microanalysis
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One-shot spectrometer for several elements using an integrated conical crystal analyzer.

Kohei Morishita1, Kouichi Hayashi, Kazuo Nakajima

  • 1Department of Socio-Environmental Energy Science, Kyoto University, Yoshida-Honmachi, Sakyo-ku, Kyoto, Japan.

The Review of Scientific Instruments
|February 4, 2012
PubMed
Summary
This summary is machine-generated.

Researchers developed a novel conical germanium crystal analyzer for time-resolved x-ray spectrometry. This one-shot spectrometer offers high efficiency and energy resolution for ultrastrong x-ray sources like free electron lasers.

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Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
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Last Updated: May 25, 2026

Quantitative Atomic-Site Analysis of Functional Dopants/Point Defects in Crystalline Materials by Electron-Channeling-Enhanced Microanalysis
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Quantitative Atomic-Site Analysis of Functional Dopants/Point Defects in Crystalline Materials by Electron-Channeling-Enhanced Microanalysis

Published on: May 10, 2021

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

Area of Science:

  • X-ray Physics
  • Spectrometry
  • Materials Science

Background:

  • Time-resolved x-ray spectrometry is a growing field, crucial for studying dynamic processes with ultrastrong x-ray sources.
  • Existing methods require advanced spectrometers capable of wide wavelength range, high efficiency, and good energy resolution for one-shot measurements.

Purpose of the Study:

  • To develop an integrated conical crystal analyzer for advanced time-resolved x-ray spectrometry.
  • To achieve a one-shot spectrometer with enhanced performance characteristics.

Main Methods:

  • Fabrication of an integrated conical germanium (Ge) crystal analyzer using a hot deformation technique.
  • The analyzer comprises multiple conical rings connected by spline surfaces for precise shaping of Ge wafers.
  • Utilized the analyzer with an alloy sample and a charge-coupled device (CCD) detector.

Main Results:

  • Simultaneous focusing of multiple characteristic x-ray lines from an alloy sample onto a CCD.
  • Achieved significantly high image brightness (100x gain compared to planar analyzers) and good spatial resolution (9-13 eV).
  • Enabled a short sample-detector distance (214.4 mm) due to the crystal's small radius of curvature (28-50 mm).

Conclusions:

  • Demonstrated the feasibility of a new focusing x-ray crystal spectrograph with controllable focal positions.
  • The developed conical Ge crystal analyzer is a promising tool for time-resolved x-ray spectrometry applications.