Related Experiment Video
Updated: May 10, 2026

12:21
Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators
Published on: April 4, 2016
Investigations of single-frequency Raman fiber amplifiers operating at 1178 nm
Iyad Dajani1, Christopher Vergien, Craig Robin
1Directed Energy Directorate, Air Force Research Laboratory, Kirtland Air Force Base, New Mexico 87117, USA.
Optics Express
|June 6, 2013
Summary
Researchers developed high-power, single-frequency Raman fiber amplifiers (RFAs). A two-stage design achieved 22 W output, overcoming limitations of single-stage systems by using tailored fiber and higher seed power.
Area of Science:
- Fiber optics
- Laser technology
- Nonlinear optics
Background:
- Single-frequency Raman fiber amplifiers (RFAs) are crucial for various applications.
- Power scaling of RFAs is often limited by nonlinear effects like stimulated Brillouin scattering (SBS).
Purpose of the Study:
- To investigate power scaling strategies for core-pumped, polarization-maintaining, single-frequency RFAs.
- To compare single-stage and two-stage RFA designs for improved output power and spectral stability.
Main Methods:
- Utilized commercial-off-the-shelf (COTS) single-mode fiber in a single-stage, counter-pumped RFA with a two-step thermal gradient to suppress SBS.
- Performed pump-probe characterization to determine the Brillouin gain spectrum (BGS) and Brillouin gain coefficient.
- Conducted fiber cutback studies to analyze signal output at the SBS threshold.
- Developed numerical simulations to predict power scaling potential with increased seed power.
- Constructed a two-stage RFA using acoustically tailored fiber with a lower Brillouin gain coefficient and higher seed power.
Main Results:
- Achieved 10 W output power at 1178 nm from a single-stage RFA using COTS fiber.
- Demonstrated a linear dependence of signal output at SBS threshold on pump power, aligning with theoretical predictions.
- Obtained 22 W of single-frequency 1178 nm output from a two-stage, counter-pumped RFA.
- Observed loss of single-frequency spectral bandwidth in a similar co-pumped two-stage RFA.
Conclusions:
- A two-stage RFA design, employing acoustically tailored fiber and higher seed power, significantly enhances output power compared to single-stage systems.
- Suppression of SBS through thermal gradients and careful fiber selection is critical for power scaling in RFAs.
- Counter-pumping configurations appear more suitable for maintaining single-frequency operation in two-stage RFAs.
Related Concept Videos
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...
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: 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...
However, a small fraction of the scattered light exhibits a frequency shift due to the exchange of energy between the incident photons and the...

