Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

325
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...
325
Raman Spectroscopy: Overview01:20

Raman Spectroscopy: Overview

360
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...
360

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Association Between Depression Subtypes and Interstitial Cystitis/Bladder Pain Syndrome.

International urogynecology journal·2026
Same author

Manifesting the connection between Laguerre-Gaussian modes and hypotrochoid modes from quantum Fock-Darwin system.

Optics express·2025
Same author

Glycerol Electro-Oxidation to Dihydroxyacetone with Coupled Hydrogen Production via In Situ Optimization of Water Oxidation Intermediates.

Small (Weinheim an der Bergstrasse, Germany)·2025
Same author

Ultrasensitive Quantification of Thyroid-Stimulating Hormone and Thyroxine by Nanoelectronic SnS<sub>2</sub> Transistor Sensors.

ACS sensors·2025
Same author

High-Pulse-Repetition-Rate Eye-Safe Raman Laser with Acousto-Optic Q-Switched Device.

Micromachines·2025
Same author

IC/BPS is not associated with bladder cancer: a nationwide propensity score matched cohort study in Taiwan.

World journal of urology·2025

Related Experiment Video

Updated: Jun 24, 2025

20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier
10:17

20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier

Published on: July 12, 2017

11.5K

Highly efficient continuous-wave solid-state Raman crystal lasers at 555 and 559 nm.

Yung-Fu Chen, Xiu-Wei Chang, Hsin-Jia Huang

    Optics Express
    |June 11, 2024
    PubMed
    Summary

    Efficient continuous-wave Raman lasers producing green and lime light at 555 and 559 nm were achieved using potassium gadolinium tungstate (KGW) and lithium triborate (LBO) crystals. High output powers of 6.6 W and 6.3 W were obtained with high conversion efficiencies.

    More Related Videos

    Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
    07:42

    Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

    Published on: December 15, 2021

    3.1K
    High-speed Continuous-wave Stimulated Brillouin Scattering Spectrometer for Material Analysis
    07:55

    High-speed Continuous-wave Stimulated Brillouin Scattering Spectrometer for Material Analysis

    Published on: September 22, 2017

    10.2K

    Related Experiment Videos

    Last Updated: Jun 24, 2025

    20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier
    10:17

    20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier

    Published on: July 12, 2017

    11.5K
    Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
    07:42

    Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

    Published on: December 15, 2021

    3.1K
    High-speed Continuous-wave Stimulated Brillouin Scattering Spectrometer for Material Analysis
    07:55

    High-speed Continuous-wave Stimulated Brillouin Scattering Spectrometer for Material Analysis

    Published on: September 22, 2017

    10.2K

    Area of Science:

    • Laser Physics
    • Nonlinear Optics
    • Solid-State Lasers

    Background:

    • Continuous-wave (CW) lasers are crucial for various scientific and industrial applications.
    • Generating visible light efficiently from near-infrared lasers remains a challenge.
    • Raman lasers offer a pathway to wavelength conversion but often suffer from efficiency limitations.

    Purpose of the Study:

    • To develop high-power, efficient CW Raman lasers operating in the green and lime spectral regions.
    • To investigate the use of Np-cut potassium gadolinium tungstate (KGW) for Stokes wave generation.
    • To optimize intracavity sum frequency generation (SFG) for visible light production.

    Main Methods:

    • Utilized a Nd:YVO4/KGW Raman laser system pumped at 1064 nm.
    • Employed Np-cut KGW crystals for Stokes wave generation at 1159 nm and 1177 nm.
    • Implemented intracavity type-I sum frequency generation in lithium triborate (LBO) crystals for 555 nm and 559 nm output.
    • Optimized cavity length and phase matching temperature for maximum conversion efficiency.

    Main Results:

    • Achieved CW output powers of 6.6 W at 555 nm and 6.3 W at 559 nm with 22 W pump power.
    • Attained high conversion efficiencies of up to 30% for 555 nm and 28.6% for 559 nm.
    • Demonstrated the effectiveness of a double-sided dichroic coating output coupler in enhancing resonance quality factor.

    Conclusions:

    • Successfully demonstrated high-power, efficient CW Raman lasers in the green and lime spectral regions.
    • The combination of KGW for Stokes generation and LBO for SFG provides a viable route for visible laser development.
    • Optimized cavity parameters are critical for achieving high performance in such laser systems.