Related Experiment Video
Updated: Jun 26, 2026

06:48
A Multimodal Wide-Field Fourier-Transform Raman Microscope
Published on: December 30, 2025
Second-harmonic-generation microsystem light source at 488 nm for Raman spectroscopy
Martin Maiwald1, Daniel Jedrzejczyk, Alexander Sahm
1Ferdinand-Braun-Institut fur Hochstfrequenztechnik, Berlin, Germany. Martin.Maiwald@FBH-Berlin.de
Optics Letters
|January 17, 2009
Summary
A compact 488 nm light source for Raman spectroscopy was developed using nonlinear frequency conversion. This efficient microsystem achieves 26% conversion efficiency and stable output, ideal for portable spectroscopic applications.
Area of Science:
- Optics and Photonics
- Materials Science
- Spectroscopy
Background:
- Microsystem light sources are crucial for portable analytical instruments.
- Efficient generation of specific wavelengths, like 488 nm, is often challenging.
- Nonlinear frequency conversion offers a pathway to compact, wavelength-specific light sources.
Purpose of the Study:
- To demonstrate a compact microsystem excitation light source emitting at 488 nm.
- To achieve efficient second-harmonic generation (SHG) for a 488 nm output.
- To develop a stable and compact light source suitable for Raman spectroscopy.
Main Methods:
- Utilized a diode laser emitting at 976 nm as the fundamental source.
- Employed a periodically poled lithium niobate (PPLN) waveguide crystal for direct single-pass nonlinear frequency conversion.
- Integrated the components onto a micro-optical bench with advanced thermal management.
Main Results:
- Achieved efficient second-harmonic generation, producing 56 mW at 488 nm from 217 mW fundamental power.
- Demonstrated a high conversion efficiency of 26% for the nonlinear process.
- The device exhibited excellent power stability below 1% and a compact footprint (25 mm x 5 mm).
Conclusions:
- A highly efficient and compact 488 nm light source was successfully realized.
- The demonstrated microsystem is wavelength-stabilized and suitable for demanding applications like Raman spectroscopy.
- This development advances the potential for portable and high-performance spectroscopic instrumentation.
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...
