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Related Concept Videos

IR Spectrometers01:25

IR Spectrometers

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...
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.
UV–Vis Spectroscopy: Woodward–Fieser Rules01:29

UV–Vis Spectroscopy: Woodward–Fieser Rules

UV–Visible absorption spectra of conjugated dienes arise from the lowest energy π → π* transitions. The light-absorbing part of the molecule is called the chromophore, and the substituents directly attached to the chromophore are called auxochromes. A strong correlation exists between the absorption maxima, λmax, and the structure of a conjugated π system. The Woodward–Fieser rules predict the value of λmax for a given structure by adding the contributions...
Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

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...
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.

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Related Experiment Video

Updated: Jun 17, 2026

Measurement of X-ray Beam Coherence along Multiple Directions Using 2-D Checkerboard Phase Grating
10:39

Measurement of X-ray Beam Coherence along Multiple Directions Using 2-D Checkerboard Phase Grating

Published on: October 11, 2016

A 4-m Asymmetric Czerny-Turner Grating Spectrograph.

J H Callomon, G G Chandler

    Applied Optics
    |January 15, 2010
    PubMed
    Summary

    A new high-resolution vacuum spectrograph was designed and built. This Czerny-Turner instrument achieves a resolving power of at least 700,000, enabling detailed spectral analysis.

    Area of Science:

    • Spectroscopy
    • Optical Engineering
    • Physics

    Background:

    • Czerny-Turner spectrographs are widely used for high-resolution spectroscopy.
    • Optimizing aberration correction is crucial for achieving high resolving power.

    Purpose of the Study:

    • To design and construct a novel high-resolution asymmetric Czerny-Turner grating vacuum spectrograph.
    • To achieve a resolving power of at least 700,000.

    Main Methods:

    • Utilized an asymmetric Czerny-Turner design with two equal-radii, non-concentric spherical mirrors.
    • Incorporated a sideways-grating translation mechanism for optimal aberration correction.
    • Employed ray tracing calculations to determine configurations for minimum aberrations.
    • Constructed a 4-meter focal length vacuum spectrograph.

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    Using Three-color Single-molecule FRET to Study the Correlation of Protein Interactions

    Published on: January 30, 2018

    Related Experiment Videos

    Last Updated: Jun 17, 2026

    Measurement of X-ray Beam Coherence along Multiple Directions Using 2-D Checkerboard Phase Grating
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    Measurement of X-ray Beam Coherence along Multiple Directions Using 2-D Checkerboard Phase Grating

    Published on: October 11, 2016

    Method for Recording Broadband High Resolution Emission Spectra of Laboratory Lightning Arcs
    07:51

    Method for Recording Broadband High Resolution Emission Spectra of Laboratory Lightning Arcs

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    11:22

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    Main Results:

    • The spectrograph was successfully designed and constructed.
    • Preliminary tests indicate a resolving power of at least 700,000 in the green spectral region.
    • High resolution was maintained across the entire 50-cm plate.

    Conclusions:

    • The developed spectrograph meets the design goals for high-resolution spectral analysis.
    • The asymmetric design and adjustable grating offer superior performance.
    • This instrument is suitable for demanding spectroscopic applications requiring exceptional resolving power.