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Related Concept Videos

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...
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...
IR Spectroscopy: Molecular Vibration Overview01:24

IR Spectroscopy: Molecular Vibration Overview

When Infrared (IR) radiation passes through a covalently bonded molecule, the bonds transition from lower to higher vibrational levels. The fundamental vibrational motions that result in infrared absorption can be classified as stretching or bending vibrations.
Stretching vibrations are vibrational motions that occur along the bond line, changing the bond length or distance between two bonded atoms. They are further distinguished as symmetric or asymmetric. In symmetric stretching, the...
Molecular Spectroscopy: Absorption and Emission01:14

Molecular Spectroscopy: Absorption and Emission

Molecules possess discrete energy levels called quantum states. Unlike atoms, which have simpler energy levels, molecules possess additional rotational and vibrational energy levels. Each energy level is separated by an energy gap, with the gaps between adjacent electronic, vibrational, and rotational levels varying significantly. The three types of energy levels in a diatomic molecule are shown in Figure 1.
IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations01:08

IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations

Identical bonds within a polyatomic group can stretch symmetrically (in-phase) or asymmetrically (out-of-phase). Similar to hydrogen bonding, these vibrations also influence the shape of the IR peak. Generally, asymmetric stretching frequencies are higher than symmetric stretching frequencies. For example, primary amines exhibit two distinct IR peaks between 3300–3500 cm−1 corresponding to the symmetric and asymmetric N-H stretching, while secondary amines exhibit a single stretching vibration...
UV–Vis Spectroscopy: Molecular Electronic Transitions01:16

UV–Vis Spectroscopy: Molecular Electronic Transitions

In Ultraviolet–Visible (UV–Vis) spectroscopy, the absorption of electromagnetic radiation is used to probe the electronic structure of molecules. This technique provides insights into molecular electronic transitions, particularly the movement of electrons between different molecular orbitals. Radiation is absorbed if the energy of the electromagnetic radiation passing through the molecule is precisely equal to the energy difference between the excited and ground states. During this process,...

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Ultrafast Time-resolved Near-IR Stimulated Raman Measurements of Functional π-conjugate Systems
09:57

Ultrafast Time-resolved Near-IR Stimulated Raman Measurements of Functional π-conjugate Systems

Published on: February 10, 2020

Stimulated Raman effect in some tetrahedral molecules.

D H Rank1, R V Wick, T A Wiggins

  • 1Physics Department, The Pennsylvania State University, University Park, Pennsylvania, USA.

Applied Optics
|January 6, 2010
PubMed
Summary
This summary is machine-generated.

Researchers studied stimulated Raman spectra in tin tetrachloride (SnCl4) and methane gas using a ruby laser. Methane showed a sharp spectral line with no pressure shift, while SnCl4 exhibited a single line and its sound velocity was measured.

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Direct Comparison of Hyperspectral Stimulated Raman Scattering and Coherent Anti-Stokes Raman Scattering Microscopy for Chemical Imaging

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Last Updated: Jun 17, 2026

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Area of Science:

  • Spectroscopy
  • Laser Physics
  • Condensed Matter Physics

Background:

  • Stimulated Raman spectroscopy (SRS) provides insights into molecular vibrations.
  • Understanding spectral line broadening and shifts is crucial for accurate molecular characterization.
  • Investigating stimulated Brillouin scattering (SBS) complements SRS studies.

Purpose of the Study:

  • To excite and analyze stimulated Raman spectra in liquid SnCl4 and methane gas.
  • To determine the vibrational frequency and pressure shift of methane.
  • To characterize the spectral features and acoustic properties of SnCl4.

Main Methods:

  • Utilizing a medium high-power ruby laser to excite stimulated Raman spectra.
  • Employing a high-resolution grating spectrograph for spectral analysis.
  • Using a Fabry-Perot etalon to observe stimulated Brillouin scattering.

Main Results:

  • Measured methane's vibrational frequency (nu1) as 2916.605 cm(-1) +/- 0.012 cm(-1) with no detectable pressure shift from 3 to 12 amagat.
  • Observed sharp, narrow stimulated Raman lines in methane, slightly broader than the laser line.
  • SnCl4 showed a single SRS Stokes line (0.5 cm(-1) width), narrower than expected, with stimulated Brillouin scattering also observed.

Conclusions:

  • Methane exhibits minimal pressure-induced spectral shifts under the studied conditions.
  • The spectral characteristics of SnCl4 suggest complex interactions influencing the stimulated Raman signal.
  • The velocity of sound in SnCl4 was determined to be 840 m/s at 27°C via stimulated Brillouin measurements.