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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...
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.

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Related Experiment Video

Updated: Jun 23, 2026

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

Low frequency Raman gain measurements using chirped pulses.

A Dogariu, D Hagan

    Optics Express
    |April 18, 2009
    PubMed
    Summary

    Researchers observed Raman gain in dielectrics using chirped femtosecond pulses. This technique measures energy transfer between light pulses, revealing material properties like Raman gain and potentially optical response times.

    Area of Science:

    • Nonlinear Optics
    • Condensed Matter Physics
    • Materials Science

    Background:

    • Two-beam coupling is a phenomenon where energy is exchanged between two light beams.
    • Raman gain describes the amplification of a probe beam due to stimulated Raman scattering.
    • Femtosecond laser pulses offer high temporal resolution for studying ultrafast phenomena.

    Purpose of the Study:

    • To observe and characterize two-beam coupling attributed to Raman gain in dielectric materials.
    • To investigate the use of chirped femtosecond pulses for probing Raman gain.
    • To explore the potential of this method for determining material optical properties.

    Main Methods:

    • Utilized a time-resolved pump-probe geometry with chirped femtosecond pulses.
    • Varied the frequency difference between the pump and probe pulses in the terahertz (THz) range.

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    Last Updated: Jun 23, 2026

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  • Measured the energy transfer between pulses as a function of temporal delay and irradiance.
  • Main Results:

    • Observed two-beam coupling mediated by stimulated Raman scattering in dielectrics (SiO2 and PbF2).
    • Quantified Raman gain for frequency detunings up to 10 THz (300 cm⁻¹).
    • Demonstrated signal dependence on the product of pump and probe irradiances, forming a dispersion-shaped curve.

    Conclusions:

    • Chirped femtosecond pulses enable effective measurement of Raman gain in dielectrics.
    • The technique provides a method for quantifying Raman gain and potentially probing electronic nonlinearities.
    • This approach may offer insights into the optical response time of bound electrons.