Рамановская спектроскопия (Раман-спектроскопия, спектроскопия комбинационного рассеяния или эффект Рамана): приборы

A Raman spectrophotometer consists of a laser source that emits focused monochromatic light, a sample holding system for various sample forms, a wavelength selector or monochromator that isolates specific wavelengths, and a detector such as a charge-coupled device or photomultiplier tube that converts optical signals into electrical ones for spectrum analysis.

Raman spectroscopy accommodates diverse sample forms including liquids, solutions, transparent solids, powders, pellets, and gases. Liquid and gaseous samples are typically tested in ordinary glass capillaries, while solids can be analyzed as powders packed in capillaries or as potassium bromide pellets, allowing flexibility in sample preparation.

Optical bandpass and notch filters remove stray laser radiation and Rayleigh scattering that interfere with the Raman signal. Fiber-optic Raman spectrometers use high-quality bandpass and notch filters to minimize Rayleigh-scattered radiation reaching the detector, ensuring accurate and clean spectral data.

The monochromator disperses scattered light into its constituent frequencies, allowing the wavelength selector to exclude all but selected individual wavelengths. This dispersal is critical for isolating the Raman signal from background noise and ensuring that only relevant spectral information reaches the detector for analysis.

Fourier-transform Raman instruments replace the monochromator with a Michelson interferometer and employ a continuous-wave laser source instead of pulsed radiation. The radiation is focused onto a cooled germanium detector for analysis, offering an alternative approach to conventional dispersive Raman spectroscopy for specific analytical applications.

The laser source emits a focused beam of monochromatic light, typically in the visible or near-infrared range, which interacts efficiently with sample molecules. This focused beam ensures that scattered light is collected effectively and directed through the wavelength selector, maximizing signal intensity and spectral resolution for accurate molecular analysis.

Charge-coupled devices and photomultiplier tubes are the most common detectors in Raman spectrophotometers, converting optical signals into electrical signals for processing. Fourier-transform Raman instruments use cooled germanium detectors instead, each detector type optimized for specific instrumental configurations and sensitivity requirements.