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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...
Confocal Fluorescence Microscopy01:16

Confocal Fluorescence Microscopy

Confocal microscopy is an advanced microscopic technique. The prime advantage of the confocal microscope over other microscopy techniques is its ability to block the out-of-focus light from the illuminated samples using pinholes. It is widely used with fluorescence optics to obtain high-resolution, sharp contrast images. Unlike optical microscopes, confocal microscopes use a focused beam of light laser to scan the entire sample surface at different z-planes. These microscopes are, therefore,...
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...
Inductively Coupled Plasma–Mass Spectrometry (ICP–MS): Overview01:19

Inductively Coupled Plasma–Mass Spectrometry (ICP–MS): Overview

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: Interference01:30

Atomic Emission Spectroscopy: Interference

In atomic emission spectroscopy (AES), high-temperature atomizers excite a broad range of elements and molecules that generate complex emissions from sources such as oxides, hydroxides, and flame combustion products in the flame or plasma. Several strategies can be employed to minimize spectral interferences caused by overlapping emission lines or bands. These include increasing instrument resolution, choosing alternative emission lines, optimally placing the detector in low-background regions,...

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Related Experiment Video

Updated: Jun 19, 2026

Investigation of Early Plasma Evolution Induced by Ultrashort Laser Pulses
11:20

Investigation of Early Plasma Evolution Induced by Ultrashort Laser Pulses

Published on: July 2, 2012

Backscattered supercontinuum emission from high-intensity laser-plasma interactions.

A Ting, K Krushelnick, H R Burris

    Optics Letters
    |October 31, 2009
    PubMed
    Summary
    This summary is machine-generated.

    High-intensity laser experiments revealed supercontinuum-like spectra in underdense plasmas due to nonlinear scattering. These findings shed light on stimulated Raman backscattering and its interaction with plasma waves.

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    Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
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    Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry

    Published on: August 1, 2017

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    Last Updated: Jun 19, 2026

    Investigation of Early Plasma Evolution Induced by Ultrashort Laser Pulses
    11:20

    Investigation of Early Plasma Evolution Induced by Ultrashort Laser Pulses

    Published on: July 2, 2012

    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

    Area of Science:

    • Plasma Physics
    • Nonlinear Optics
    • Laser-Plasma Interactions

    Background:

    • Understanding nonlinear scattering mechanisms is crucial for controlling laser-plasma interactions.
    • Previous studies have explored stimulated Raman scattering but lacked detailed spectral analysis at high intensities.

    Purpose of the Study:

    • To investigate nonlinear scattering mechanisms in underdense plasmas using high-intensity subpicosecond laser pulses.
    • To characterize the spectral features of stimulated Raman backscattering at intensities up to 2 x 10^18 W/cm^2.

    Main Methods:

    • Experiments involving high-intensity subpicosecond laser pulses interacting with underdense plasmas.
    • Spectroscopic analysis of backscattered light to examine spectral broadening and modulations.

    Main Results:

    • Observed an extremely broad, supercontinuum-like stimulated Raman backscattered spectrum (Deltaomega/omega(0) > 1).
    • The spectrum extended from approximately 500 nm to over 1200 nm, limited by detector sensitivity.
    • Measured large-amplitude modulations within the backscattered spectrum.

    Conclusions:

    • The broad spectrum is attributed to nonlinear scattering processes in the plasma.
    • Modulations are likely caused by the interaction of stimulated Raman scattered light with ion plasma waves.