Related Experiment Video
Updated: Jun 20, 2026

10:17
20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier
Published on: July 12, 2017
High-efficiency joule-level Raman generation in Pb vapor
Optics Letters
|August 28, 2009
Summary
Researchers achieved high-energy blue-green laser output using Raman shifting of an injection-locked XeCl laser in lead vapor. This demonstrates a promising pathway for efficient blue-green laser generation with potential for over 1.4% efficiency.
Area of Science:
- Laser Physics
- Nonlinear Optics
- Atomic Vapor Lasers
Background:
- High-power blue-green lasers are crucial for various applications, including remote sensing and underwater communications.
- Raman shifting offers a method to convert existing laser wavelengths to desired spectral regions.
- Lead (Pb) vapor is an effective medium for efficient Raman conversion of UV laser sources.
Purpose of the Study:
- To demonstrate efficient blue-green radiation generation via Raman shifting of an injection-locked XeCl laser.
- To investigate the energy conversion efficiency of the XeCl/Pb Raman laser system.
- To assess the potential for high overall laser efficiency in this system.
Main Methods:
- Utilizing an injection-locked XeCl laser operating in the ultraviolet (UV) spectrum.
- Employing lead (Pb) vapor as the Raman gain medium.
- Measuring the output energy and spectral characteristics of the generated blue-green radiation.
Main Results:
- Achieved nearly 1 Joule of blue-green radiation output.
- Generated radiation in 60-nanosecond (nsec) pulses.
- Observed a 50% Raman energy conversion efficiency in both oscillator and oscillator-amplifier configurations.
Conclusions:
- The XeCl/Pb system demonstrates a viable route for efficient blue-green laser generation.
- The high conversion efficiency suggests a potential for exceeding 1.4% overall XeCl/Pb blue-green laser efficiency.
- Further optimization could lead to practical high-energy blue-green laser sources.
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...
Atomic Absorption Spectroscopy: Atomization Methods
Atomic Absorption Spectroscopy (AAS) atomizes samples through flame atomization or electrothermal atomization. Flame atomization typically involves a nebulizer and spray chamber assembly to combine the sample with a fuel–oxidant mixture, creating a fine aerosol mist that enters a burner. Typically, the fuel and oxidant are combined in an approximately stoichiometric ratio. However, for atoms that are easily oxidized, a fuel-rich mixture may be more advantageous. Only about 5% of the aerosol...
Atomic Absorption Spectroscopy: Radiation and Light Sources
Atomic absorption spectroscopy (AAS) relies on the Beer-Lambert law, which requires that the radiation source emits a narrow range of wavelengths to match the absorption characteristics of the analyte atom. The primary criteria for choosing an appropriate radiation source in AAS is to provide a precise and intense emission at specific wavelengths that will allow accurate detection of the analyte.
Two common narrow-range 'line' sources used in AAS are hollow-cathode lamps (HCLs) and...
Two common narrow-range 'line' sources used in AAS are hollow-cathode lamps (HCLs) and...
Joule-Thomson Effect
The Joule-Thomson effect, also known as the Joule-Kelvin effect, describes the temperature change of a fluid when it is forced through a valve or porous plug while keeping it in a thermally insulated environment. This experiment is called a throttling process. This is an important effect widely used in refrigeration and the liquefaction of gases.
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
UV–Vis Spectroscopy: Molecular Electronic Transitions
In Ultraviolet–Visible (UV–Vis) spectroscopy, the absorption of electromagnetic radiation is used to probe the electronic structure of molecules. This technique provides insights into molecular electronic transitions, particularly the movement of electrons between different molecular orbitals. Radiation is absorbed if the energy of the electromagnetic radiation passing through the molecule is precisely equal to the energy difference between the excited and ground states. During this process,...

