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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...
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...
NMR Spectrometers: Resolution and Error Correction01:14

NMR Spectrometers: Resolution and Error Correction

When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
Atomic Absorption Spectroscopy: Interference01:25

Atomic Absorption Spectroscopy: Interference

Interference leads to systematic error in atomic absorption (AA) measurements by enhancing or diminishing the analytical signal or the background. These interferences can be grouped into three main categories: spectral interference, chemical interference, and physical interference.
Spectral interference occurs when signals from other elements or molecules overlap with the analyte signal, falsely elevating or masking the analyte's absorbance. This interference can be corrected using Zeeman,...
¹H NMR Signal Integration: Overview00:58

¹H NMR Signal Integration: Overview

The intensity of a signal, which can be represented by the area under the peak, depends on the number of protons contributing to that signal. The area under each peak is shown as a vertical line called an integral, with the integral value listed under it, as seen in the proton NMR spectrum of benzyl acetate. Each integral value is divided by the smallest integral value to obtain the ratio of the number of protons producing each signal. The ratio reveals the relative number of protons and not...

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Ultrafast Time-resolved Near-IR Stimulated Raman Measurements of Functional π-conjugate Systems
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Requirements for relative intensity correction of Raman spectra obtained by column-summing charge-coupled device

Wilbur S Hurst1, Steven J Choquette, Edgar S Etz

  • 1Chemical Science and Technology Laboratory, National Institute of Standards and Technology, Gaithersburg, Maryland 20899, USA. wilbur.hurst@nist.gov

Applied Spectroscopy
|August 21, 2007
PubMed
Summary

Accurate Raman spectra intensity correction requires careful consideration of charge-coupled device (CCD) detector operation. Summing CCD pixel rows can introduce spectral distortions if the light source

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Last Updated: Jul 13, 2026

Ultrafast Time-resolved Near-IR Stimulated Raman Measurements of Functional π-conjugate Systems
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Resolving Water, Proteins, and Lipids from In Vivo Confocal Raman Spectra of Stratum Corneum through a Chemometric Approach
09:32

Resolving Water, Proteins, and Lipids from In Vivo Confocal Raman Spectra of Stratum Corneum through a Chemometric Approach

Published on: September 26, 2019

Area of Science:

  • Spectroscopy
  • Analytical Chemistry
  • Instrumentation

Background:

  • Relative intensity correction is crucial for accurate Raman spectra analysis.
  • Raman spectrometers often utilize two-dimensional charge-coupled device (CCD) array detectors.
  • CCD detectors can operate in different modes, including summing pixel rows.

Purpose of the Study:

  • To investigate the impact of CCD row summing on Raman spectra intensity correction.
  • To identify restrictions on light source spatial intensity profiles for accurate correction.
  • To quantify potential spectral distortions introduced by the row summing method.

Main Methods:

  • Development of numerical expressions to define restrictions for accurate intensity correction.
  • Modeling of different cases to estimate the magnitude of spectral distortions.
  • Analysis of inherent pixel quantum efficiency variations in CCD detectors.
  • Evaluation of spectral effects caused by localized pixel quantum efficiency changes.

Main Results:

  • Operation mode where CCD rows are summed imposes specific spatial intensity profile requirements on the calibration light source.
  • These requirements can also extend to the spatial intensity profile of the measured Raman signal.
  • Significant spectral distortions can arise when these restrictions are not met, particularly with non-uniform pixel quantum efficiency.

Conclusions:

  • Proper selection and characterization of the irradiance source are critical for accurate Raman spectra.
  • Understanding CCD detector spatial response and pixel quantum efficiency is essential to avoid spectral artifacts.
  • The study provides a framework for deriving and applying constraints to ensure reliable intensity correction.