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 Spectrometers01:16

Mass Spectrometers

10.9K
This lesson details the instrumentation of a mass spectrometer—a physical instrument to perform mass spectrometry on analyte molecules and record the characteristic mass spectra. This is achieved via three chief functions:
10.9K
Tandem Mass Spectrometry01:21

Tandem Mass Spectrometry

3.0K
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...
3.0K
Mass Analyzers: Common Types01:19

Mass Analyzers: Common Types

1.9K
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...
1.9K
Mass Spectrometry: Overview01:19

Mass Spectrometry: Overview

10.5K
Mass spectrometry is an analytical technique used to determine the molecular mass and molecular formula of a compound. The basic principle of mass spectrometry is to generate ions from the analyte molecule and measure these ion abundances against their molecular mass. One common type of ionization, known as electron ionization or EI, bombards the analyte molecules in the gas phase with high-energy electron beams. The electron beams displace an electron from the molecule and leave behind a...
10.5K
Atomic Emission Spectroscopy: Instrumentation01:22

Atomic Emission Spectroscopy: Instrumentation

1.6K
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.
1.6K
Mass Analyzers: Overview01:13

Mass Analyzers: Overview

2.1K
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...
2.1K

You might also read

Related Articles

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

Sort by
Same author

Heme oxygenase-mediated resistance to oxygen toxicity in hamster fibroblasts.

The Journal of biological chemistry·1997
Same author

Novel and frequent mutations of hepatitis B virus coincide with a major histocompatibility complex class I-restricted T-cell epitope of the surface antigen.

Journal of virology·1997
Same author

Ras p21 protein immunoreactivity and its relationship to p53 expression and prognosis in gallbladder and extrahepatic biliary carcinoma.

European journal of surgical oncology : the journal of the European Society of Surgical Oncology and the British Association of Surgical Oncology·1997
Same author

On-line micellar electrokinetic chromatography-electrospray ionization mass spectrometry using anodically migrating micelles.

Analytical chemistry·1997
Same author

Lamotrigine trial in idiopathic parkinsonism: a double-blind, placebo-controlled, crossover study.

Neurology·1997
Same author

Involution of the sheep mammary gland.

Journal of anatomy·1997

Related Experiment Video

Updated: Apr 4, 2026

Quantification of Hydrogen Concentrations in Surface and Interface Layers and Bulk Materials through Depth Profiling with Nuclear Reaction Analysis
14:11

Quantification of Hydrogen Concentrations in Surface and Interface Layers and Bulk Materials through Depth Profiling with Nuclear Reaction Analysis

Published on: March 29, 2016

27.8K

CNS active target (CAT) for missing mass spectroscopy with intense beams.

S Ota1, H Tokieda1, C S Lee2

  • 1Center for Nuclear Study, The University of Tokyo, 2-1 Hirosawa, Wako, Saitama 351-0198 Japan.

Journal of Radioanalytical and Nuclear Chemistry
|August 29, 2015
PubMed
Summary

A novel gaseous active target, the CAT (Compton Anisotropy Telescope), utilizes a dual gain THGEM detector. This innovation allows simultaneous detection of high-intensity beam and recoil particles within a wide dynamic range.

Keywords:
Active targetDeuteriumGas targetTHGEMTime projection chamber

More Related Videos

Automated Delivery of Microfabricated Targets for Intense Laser Irradiation Experiments
06:40

Automated Delivery of Microfabricated Targets for Intense Laser Irradiation Experiments

Published on: January 28, 2021

4.8K
High-Resolution Neutron Spectroscopy to Study Picosecond-Nanosecond Dynamics of Proteins and Hydration Water
08:48

High-Resolution Neutron Spectroscopy to Study Picosecond-Nanosecond Dynamics of Proteins and Hydration Water

Published on: April 28, 2022

2.3K

Related Experiment Videos

Last Updated: Apr 4, 2026

Quantification of Hydrogen Concentrations in Surface and Interface Layers and Bulk Materials through Depth Profiling with Nuclear Reaction Analysis
14:11

Quantification of Hydrogen Concentrations in Surface and Interface Layers and Bulk Materials through Depth Profiling with Nuclear Reaction Analysis

Published on: March 29, 2016

27.8K
Automated Delivery of Microfabricated Targets for Intense Laser Irradiation Experiments
06:40

Automated Delivery of Microfabricated Targets for Intense Laser Irradiation Experiments

Published on: January 28, 2021

4.8K
High-Resolution Neutron Spectroscopy to Study Picosecond-Nanosecond Dynamics of Proteins and Hydration Water
08:48

High-Resolution Neutron Spectroscopy to Study Picosecond-Nanosecond Dynamics of Proteins and Hydration Water

Published on: April 28, 2022

2.3K

Area of Science:

  • Nuclear Physics
  • Particle Detectors
  • Experimental Physics

Background:

  • Active targets are crucial for studying nuclear reactions.
  • Time projection chambers (TPCs) offer 3D tracking capabilities.
  • Detecting both beam and recoil particles simultaneously is challenging, especially at high beam intensities.

Purpose of the Study:

  • To introduce a new gaseous active target detector named CAT.
  • To present a novel dual gain THGEM (Thick Gas Electron Multiplier) technology.
  • To enable simultaneous detection of beam and recoil particles with a wide dynamic range.

Main Methods:

  • Development of a gaseous active target based on a time projection chamber (TPC).
  • Implementation of a dual gain THGEM structure.
  • Measurement of effective gain in low and high gain regions.

Main Results:

  • The CAT detector effectively reduces gain for beam particles while maintaining high gain for recoil particles.
  • The measured effective gain in the low gain region was 100 times smaller than in the high gain region.
  • The detector demonstrated a wide dynamic range, capable of handling beam intensities > 10^5 Hz.

Conclusions:

  • The dual gain THGEM technology in the CAT detector significantly enhances its dynamic range.
  • This advancement allows for simultaneous detection of beam and recoil particles in high-intensity experiments.
  • The CAT detector is a promising tool for future nuclear physics research.