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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...
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...
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.
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Mass Spectrometers

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:
Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

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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...
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Mass Analyzers: Overview

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...

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The instrument function of a wide angle Michelson interferometer spectrometer.

W D Johnston1

  • 1NASA, Goddard Space Flight Center,Greenbelt, Maryland 20771, USA.

Applied Optics
|January 12, 2010
PubMed
Summary

This study introduces a new method for wide-angle Michelson interferometer spectrometers, enhancing field of view and reducing interfaces. The instrument

Area of Science:

  • Optics and Photonics
  • Spectroscopy
  • Interferometry

Background:

  • Conventional Michelson interferometers face limitations in field of view and optical complexity.
  • Developing advanced spectroscopic instruments is crucial for various scientific applications.

Purpose of the Study:

  • To derive the instrument function for a wide-angle Michelson interferometer spectrometer.
  • To explore a novel method for computing phase differences in interferometric systems.
  • To investigate the impact of material properties and field of view on instrument performance.

Main Methods:

  • A novel computational approach was used to determine the phase difference between interfering beams.
  • The instrument function was derived using easily measurable parameters.

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  • A working model was constructed to validate theoretical findings.
  • Main Results:

    • The derived instrument function is expressed in terms of known or measurable optical properties.
    • The interferometer design achieves optical immersion using solid materials, reducing reflective interfaces.
    • A linear relationship was identified between the allowable field of view and the refractive index of the cube material.
    • Experimental validation produced clear fringes using both white light and mercury green light.

    Conclusions:

    • The novel method provides an effective way to characterize wide-angle Michelson interferometer spectrometers.
    • Solid immersion designs offer significant advantages in field of view and optical efficiency.
    • The findings enable the design of more versatile and high-performance spectroscopic instruments.