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

Inductively Coupled Plasma Atomic Emission Spectroscopy: Principle01:19

Inductively Coupled Plasma Atomic Emission Spectroscopy: Principle

Inductively coupled plasma (ICP) is the most widely used plasma source in atomic emission spectroscopy (AES), also known as Inductively Coupled Plasma Optical Emission Spectroscopy (ICP-OES). The ICP source, or torch, consists of three concentric quartz tubes with argon gas flowing through them. A spark from a Tesla coil initiates the ionization of argon, generating a high-temperature plasma.
The ions and electrons produced interact with the fluctuating magnetic field created by a water-cooled...
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 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.
Gas Chromatography: Types of Detectors-II01:19

Gas Chromatography: Types of Detectors-II

In gas chromatography, different detectors are employed to meet specific analytical needs. These detectors are often categorized based on their detection mechanisms and the types of compounds they are best suited to analyze. Thermal Conductivity Detectors (TCD), Flame Ionization Detectors (FID), and Electron Capture Detectors (ECD) represent common categories, each with unique operating principles and applications. However, beyond these, several other detectors are designed for more specialized...
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 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.

You might also read

Related Articles

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

Sort by
Same author

The New Scanning Mode in Digital Linear Ion Trap Mass Spectrometry for the Detection of New Psychoactive Substances in E-Cigarette Oils.

Analytical chemistry·2026
Same author

Development of Tandem Ion Mobility Spectrometry Based on Heat-Induced Dissociation and Its Application in Explosives Detection.

Analytical chemistry·2025
Same author

Direct Implementation of MS<sup>n</sup> Using Frequency Scanning Collision Induced Dissociation in a Digital Ion Trap Mass Spectrometer.

Journal of the American Society for Mass Spectrometry·2024
Same author

Development of an Ion Mobility Spectrometer Based on a Pulsed Photoelectric Effect Ionization Source.

Analytical chemistry·2024
Same author

Direct Performance of Triple-Stage Tandem Mass Spectrometry Analysis Using Dual-Direction Dipolar Excitation in a Digital Linear Ion Trap.

Journal of the American Society for Mass Spectrometry·2024
Same author

Detection of Trace Explosives Using a Novel Sample Introduction and Ionization Method.

Molecules (Basel, Switzerland)·2022

Related Experiment Video

Updated: Jul 6, 2026

Quantitative Detection of Trace Explosive Vapors by Programmed Temperature Desorption Gas Chromatography-Electron Capture Detector
07:57

Quantitative Detection of Trace Explosive Vapors by Programmed Temperature Desorption Gas Chromatography-Electron Capture Detector

Published on: July 25, 2014

Air-Based Porous Array Dielectric Barrier Discharge Ionization Source for Explosive Trace Detection.

Tianyi Zhao1, Jie Ren1, Zihang Jia1

  • 1School of Electronic and Information Engineering, Soochow University, Suzhou 215006, China.

Analytical Chemistry
|July 4, 2026
PubMed
Summary

A new atmospheric pressure ionization source using dielectric barrier discharge (DBD) offers sensitive explosive trace detection. This compact, reagent-free technology enhances safety and security screening.

More Related Videos

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F&#8722;
06:53

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−

Published on: July 27, 2018

Additive Manufacturing-Enabled Low-Cost Particle Detector
06:05

Additive Manufacturing-Enabled Low-Cost Particle Detector

Published on: March 24, 2023

Related Experiment Videos

Last Updated: Jul 6, 2026

Quantitative Detection of Trace Explosive Vapors by Programmed Temperature Desorption Gas Chromatography-Electron Capture Detector
07:57

Quantitative Detection of Trace Explosive Vapors by Programmed Temperature Desorption Gas Chromatography-Electron Capture Detector

Published on: July 25, 2014

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F&#8722;
06:53

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−

Published on: July 27, 2018

Additive Manufacturing-Enabled Low-Cost Particle Detector
06:05

Additive Manufacturing-Enabled Low-Cost Particle Detector

Published on: March 24, 2023

Area of Science:

  • Analytical Chemistry
  • Mass Spectrometry
  • Materials Science

Background:

  • Explosive trace detection (ETD) is crucial for security applications.
  • Existing methods often face limitations in sensitivity, portability, or operational complexity.
  • Atmospheric pressure ionization sources are desirable for field deployable mass spectrometry.

Purpose of the Study:

  • To propose and validate a novel atmospheric pressure ionization source for explosive trace detection.
  • To balance practical application requirements with high detection performance.
  • To develop a compact, efficient, and reagent-free ionization source for next-generation ETD.

Main Methods:

  • Development of a porous array dielectric barrier discharge (DBD) ionization source on a printed circuit board (PCB).
  • Utilized air as the discharge gas with a countercurrent gas flow system.
  • Employed pulsed discharge operation to reduce interference, power consumption, and enhance source lifetime.

Main Results:

  • Achieved large-area discharge with ion currents exceeding 300 nA, improving ion generation efficiency.
  • Countercurrent gas flow effectively mitigated ozone and nitrogen oxide interference.
  • Demonstrated good linear response over two orders of magnitude for nitro explosives (TNT, RDX, etc.) using a miniature digital linear ion trap mass spectrometer, with a low detection limit (0.0025 ng for 2,4-DNT).

Conclusions:

  • The proposed DBD ionization source offers a compact, soft ionization method for explosive trace detection.
  • The design eliminates the need for additional reagents or consumable gases, simplifying operation.
  • This technology presents a feasible solution for advancing mass-spectrometry-based explosive trace detection systems.