|
||
|
Dispersive Raman spectrometers measure the wavelength and intensity of inelastically-scattered light. They use visible lasers, a grating, and charged-coupled detectors (CCD) to collect data. In most dispersive Raman spectrometers, the CCD is a silicon array. The laser acts as a light source and irradiates the sample. In a process known as Rayleigh scattering, most of the radiation elastically scatters or "reflects off" the sample at the same energy as the incoming laser radiation. Nevertheless, a small amount (approximately one photon out of a million, or 0.00001%) scatters from the sample at a wavelength that is slightly shifted from the original wavelength. Products & Services
Infrared (IR) spectrometers measure the wavelength and intensity of the absorption of infrared light by a sample.
Raman spectrometers are used to measure the wavelength and intensity of inelastically scattered light from molecules. They can determine the chemical composition of a sample based on its wavelength and intensity.
Spectrometers are analytical instruments which disperse an emission (such as particles or radiation) according to some property of the emission (such as mass or energy) in order to measure the amount of the dispersion. This product area includes visible, infrared (IR), ultraviolet (UV), atomic absorption (AA), optical emission (OE), Raman, X-ray fluorescence (XRF) and mass spectrometers. Specific search forms are also available.
UV and visible spectrometers measure the amount of ultraviolet (UV) and visible light transmitted or absorbed by a sample placed in the spectrometer.
Specialty or proprietary products and accessories related to spectrometers.
Product Announcements
Topics of Interest
3.2 Fourier Transform Near-Infrared Raman Spectroscopy
3.2.1 Theory
Raman spectroscopy is an emission technique which involves irradiating a sample with a laser and collecting the scattered...
(Read More)
The turbidity, ?, expressed in m ?1, is a measure of the total intensity of light, I, scattered in all directions from an incoming beam of intensity I o. A typical data table and the mathematical...
(Read More)
11.1 Raman, Brillouin, Rayleigh, and Mie Scattering
As early as 1923, Einstein generalized the notion of stimulated and spontaneous emission to a new kind of light scattering process, in which the...
(Read More)
3.2 Diffraction Gratings and Tunable Filter Spectrometers
A light source can be decomposed into its spectral constituents by either dividing the spectrum over space in a dispersive configuration or...
(Read More)
4.4.2 Optical Amplifiers and Regenerators
4.4.2.1 Amplifiers
In Chapter 2 (Section 2.17), we described the physics and technology of optical amplification. Amplification is required to overcome signal...
(Read More)
|
|