Related Experiment Video
Updated: Jul 31, 2025

10:42
Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
Published on: May 3, 2019
6.8K
Below-threshold harmonic generation in gas-jets for Th-229 nuclear spectroscopy
Optics Express
|May 9, 2023
Summary
Generating vacuum ultra-violet (VUV) frequency combs using below-threshold harmonic generation in gas jets shows promise for probing the Thorium-229 isotope. Researchers achieved significant conversion efficiencies for VUV harmonics, crucial for developing new VUV light sources.
Area of Science:
- Atomic, Molecular, and Optical Physics
- Quantum Optics
- Laser Physics
Background:
- Below-threshold harmonic generation in gas jets is a key method for producing vacuum ultra-violet (VUV) light.
- VUV light sources are essential for applications like probing nuclear isomeric transitions, such as that of Thorium-229.
- Developing efficient VUV frequency combs requires understanding harmonic generation efficiencies.
Purpose of the Study:
- To measure the conversion efficiencies of below-threshold harmonics generated in Argon and Krypton gas jets.
- To assess the potential of Ytterbium-based laser sources for generating VUV frequency combs.
- To provide crucial data for the development of practical VUV light sources.
Main Methods:
- Utilized a phase-mismatched generation scheme with Argon and Krypton as nonlinear media.
- Employed a 220 fs, 1030 nm Ytterbium laser source to generate 7th and 5th harmonics.
- Characterized the 3rd harmonic generation from a 178 fs, 515 nm laser source.
Main Results:
- Achieved a maximum conversion efficiency of 1.1 × 10⁻⁵ for the 7th harmonic (147 nm) using the 1030 nm source.
- Obtained a maximum conversion efficiency of 0.78 × 10⁻⁴ for the 5th harmonic (206 nm).
- Measured a maximum conversion efficiency of 0.3% for the 3rd harmonic (172 nm) from the 515 nm source.
Conclusions:
- Below-threshold harmonic generation in gas jets is a viable route to VUV frequency combs.
- The measured efficiencies are critical for designing and optimizing VUV sources for spectroscopic applications.
- This work advances the development of VUV light sources for fundamental science and potential applications.
Related Concept Videos
Emission Spectra
56.5K
When solids, liquids, or condensed gases are heated sufficiently, they radiate some of the excess energy as light. Photons produced in this manner have a range of energies, and thereby produce a continuous spectrum in which an unbroken series of wavelengths is present.
56.5K
Atomic Emission Spectroscopy: Interference
237
In atomic emission spectroscopy (AES), high-temperature atomizers excite a broad range of elements and molecules that generate complex emissions from sources such as oxides, hydroxides, and flame combustion products in the flame or plasma. Several strategies can be employed to minimize spectral interferences caused by overlapping emission lines or bands. These include increasing instrument resolution, choosing alternative emission lines, optimally placing the detector in low-background regions,...
237
Atomic Emission Spectroscopy: Instrumentation
548
The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers. Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
548
Nuclear Transmutation
17.7K
Nuclear transmutation is the conversion of one nuclide into another. It can occur by the radioactive decay of a nucleus, or the reaction of a nucleus with another particle. The first manmade nucleus was produced in Ernest Rutherford’s laboratory in 1919 by a transmutation reaction, the bombardment of one type of nuclei with other nuclei or with neutrons. Rutherford bombarded nitrogen-14 atoms with high-speed α particles from a natural radioactive isotope of radium and observed...
17.7K
Atomic Absorption Spectroscopy: Radiation and Light Sources
452
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...
452
Atomic Absorption Spectroscopy: Atomization Methods
595
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...
595

