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Related Concept Videos

IR Spectrometers01:25

IR Spectrometers

2.7K
There are two main infrared (IR) spectrophotometers: dispersive IR spectrometers and Fourier transform infrared (FTIR) spectrometers. In a dispersive IR spectrometer, a beam of infrared radiation produced by a hot wire is divided into two parallel equal-intensity beams using mirrors. One beam passes through the sample, while another is a reference beam. The beams then move through the monochromator, which separates the radiations into a continuous spectrum of different frequencies. The...
2.7K
Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation01:26

Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation

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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....
796
Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

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A conventional Raman spectrophotometer includes a laser source, a sample holding system, a wavelength selector, and a detector.
The monochromatic laser source, typically using visible or near-infrared radiation, generates a highly focused beam of light. This light interacts with the molecules of the sample, scattering some of the light. Liquid and gaseous samples are usually tested in ordinary glass capillaries, while solids can be analyzed as powders packed in capillaries or as potassium...
1.4K
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

1.8K
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...
1.8K
Atomic Emission Spectroscopy: Instrumentation01:22

Atomic Emission Spectroscopy: Instrumentation

1.3K
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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Related Experiment Video

Updated: Feb 16, 2026

Direct Comparison of Hyperspectral Stimulated Raman Scattering and Coherent Anti-Stokes Raman Scattering Microscopy for Chemical Imaging
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Direct Comparison of Hyperspectral Stimulated Raman Scattering and Coherent Anti-Stokes Raman Scattering Microscopy for Chemical Imaging

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Computational reconfigurable imaging spectrometer.

R M Sullenberger, A B Milstein, Y Rachlin

    Optics Express
    |December 17, 2017
    PubMed
    Summary
    This summary is machine-generated.

    We developed a new hyperspectral imaging spectrometer using computational imaging. This system allows sensitive measurements with smaller, cheaper components, ideal for size-constrained platforms.

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    Area of Science:

    • Optics and Photonics
    • Computational Imaging
    • Spectroscopy

    Background:

    • Hyperspectral imaging spectrometers are crucial for various applications but often require large, expensive components.
    • Existing systems face limitations in size, weight, and power (SWaP) for deployment on small platforms.
    • There is a need for compact, cost-effective hyperspectral imaging solutions.

    Purpose of the Study:

    • To demonstrate a novel hyperspectral imaging spectrometer utilizing computational imaging techniques.
    • To enable sensitive spectral measurements using smaller, less expensive components.
    • To meet the stringent SWaP requirements of small space and air platforms.

    Main Methods:

    • The developed system is a computational reconfigurable imaging spectrometer (CRISP).
    • It employs a spectrally coded focal-plane mask and platform motion to modulate the optical spectrum.
    • This modulation allows for the simultaneous measurement of multiple spectral bins.

    Main Results:

    • The CRISP system enables sensitive measurements from smaller, noisier, and less-expensive components like uncooled microbolometers.
    • The system successfully demodulates coded patterns to reconstruct an optical spectrum for each pixel.
    • This approach overcomes limitations of traditional hyperspectral imaging systems.

    Conclusions:

    • The novel computational hyperspectral imaging spectrometer offers a viable solution for SWaP-constrained applications.
    • This technology can significantly expand the use of hyperspectral imaging in micro-satellite, UAV, and handheld devices.
    • Further development could lead to even more compact and versatile spectral imaging instruments.