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Related Concept Videos

Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

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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...
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Raman Spectroscopy: Overview01:20

Raman Spectroscopy: Overview

2.6K
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...
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IR Spectroscopy: Molecular Vibration Overview01:24

IR Spectroscopy: Molecular Vibration Overview

5.8K
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...
5.8K
IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration01:16

IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration

3.3K
A covalently bonded heteronuclear diatomic molecule can be modeled as two vibrating masses connected by a spring. The vibrational frequency of the bond can be expressed using an equation derived from Hooke's law, which describes how the force applied to stretch or compress a spring is proportional to the displacement of the spring. In this case, the atoms behave like masses, and the bond acts like a spring.
According to Hooke's law, the vibrational frequency is directly proportional to...
3.3K
IR Spectrum Peak Broadening: Hydrogen Bonding01:23

IR Spectrum Peak Broadening: Hydrogen Bonding

1.9K
The vibrational frequency of a bond is directly proportional to its bond strength. As a result, stronger bonds vibrate at higher frequencies, while weaker bonds vibrate at lower frequencies. The stretching vibration of the strong O–H bond in alcohols and phenols (very dilute solution or gas phase) appears as a sharp peak at 3600–3650 cm−1.
However, the extent of hydrogen bonding influences the observed stretching frequency and band broadening. Intermolecular or intramolecular...
1.9K
IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations01:08

IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations

2.0K
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...
2.0K

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A Multimodal Wide-Field Fourier-Transform Raman Microscope
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Spectral broadening in continuous-wave intracavity Raman lasers.

Gerald M Bonner, Jipeng Lin, Alan J Kemp

    Optics Express
    |April 11, 2014
    PubMed
    Summary

    Spectral broadening in Raman lasers was studied. Limiting the fundamental spectrum with etalons improved output power by narrowing the spectral peak.

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    Area of Science:

    • Laser Physics
    • Nonlinear Optics

    Background:

    • Intracavity Raman lasers are crucial for generating specific wavelengths.
    • Spectral broadening of the fundamental field can affect laser performance.
    • Understanding this broadening is key to optimizing laser output.

    Purpose of the Study:

    • Investigate spectral broadening of the fundamental field in intracavity Raman lasers.
    • Analyze the impact of spectral broadening on Raman gain.
    • Explore methods to control spectral width for improved power.

    Main Methods:

    • Comparative analysis of two Raman lasers with different Raman crystal linewidths.
    • Theoretical discussion of the spectral broadening mechanism.
    • Experimental exploration of etalon use to limit spectral width.

    Main Results:

    • Spectral broadening was observed and its mechanism discussed.
    • The effect of broadening varied with different Raman linewidths.
    • Using etalons to narrow the fundamental spectrum significantly improved output power.

    Conclusions:

    • Spectral broadening negatively impacts effective Raman gain.
    • Etalons are effective in limiting the fundamental spectrum to a single peak.
    • Controlling spectral width via etalons leads to enhanced laser output power.