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Related Concept Videos

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...
UV–Vis Spectrometers01:14

UV–Vis Spectrometers

The absorbance of UV and visible (UV–visible) radiations is measured using a UV–visible spectrophotometer. Deuterium lamps, which emit UV radiation, and tungsten lamps, which produce radiation in the visible region, are used as light sources in UV–visible spectrophotometers. A monochromator or prism is used for diffraction grating, i.e., to split the incoming radiation into different wavelengths. A system of slits is used to focus the desired wavelength on the sample cell. Samples for...
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...
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

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...
Raman Spectroscopy: Overview01:20

Raman Spectroscopy: Overview

The underlying principle of Raman spectroscopy is based on the interaction between light and matter, specifically molecules' inelastic scattering of photons. When a monochromatic beam of light, typically from a laser source, interacts with a sample, most scattered light has the same frequency as the incident light. This is known as Rayleigh scattering.
However, a small fraction of the scattered light exhibits a frequency shift due to the exchange of energy between the incident photons and the...
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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High Speed Sub-GHz Spectrometer for Brillouin Scattering Analysis
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Published on: December 22, 2015

A Tunable Catadioptric Spectrometer with Bragg-Condition-Preserving Rotation for High-Resolution Spectroscopy.

Zhongyi Yao1, Shuoying Ren1, Xinbing Wang1

  • 1Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan 430074, China.

Sensors (Basel, Switzerland)
|May 13, 2026
PubMed
Summary
This summary is machine-generated.

This study introduces a new tunable catadioptric spectrometer using a volume phase holographic (VPH) grating and a reflector. This novel design achieves both high spectral resolution and broad wavelength tunability for advanced spectroscopy applications.

Keywords:
Raman spectroscopytransmission spectrometertunable catadioptric spectrometervolume phase holographic grating

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Area of Science:

  • Optics and Photonics
  • Spectroscopy
  • Instrument Development

Background:

  • Conventional transmission spectrometers have fixed configurations, limiting simultaneous high spectral resolution and broad wavelength coverage.
  • Volume Phase Holographic (VPH) grating spectrometers offer high throughput but often lack tunability.
  • There is a need for compact, tunable spectrometers that maintain high performance across a wide spectral range.

Purpose of the Study:

  • To theoretically analyze and experimentally validate a novel tunable catadioptric transmission spectrometer.
  • To demonstrate simultaneous achievement of high spectral resolution and broad wavelength tunability.
  • To showcase the application of the spectrometer in resolving closely spaced spectral features.

Main Methods:

  • Developed a catadioptric grating assembly combining a VPH grating and a planar reflector with synchronous rotation for wavelength scanning.
  • Theoretically derived optical configuration and structural parameters for optimal performance.
  • Constructed a prototype spectrometer and performed spectral response and resolution measurements.

Main Results:

  • The prototype spectrometer demonstrated wavelength tunability from 410 nm to 650 nm by adjusting the rotation angle.
  • High diffraction efficiency was maintained across the entire tuning range.
  • Achieved spectral resolutions of 0.1 nm (2400 g/mm) and 0.18 nm (1500 g/mm).
  • Successfully resolved closely spaced Raman peaks of CH4 and C2H6 in gas Raman spectroscopy.

Conclusions:

  • The proposed tunable catadioptric spectrometer effectively combines excellent wavelength tunability with high spectral resolution.
  • This novel design overcomes the limitations of conventional fixed-configuration spectrometers.
  • The spectrometer shows significant potential for applications requiring precise spectral analysis, such as gas spectroscopy.