Related Experiment Video
Updated: Apr 13, 2026

09:39
In-situ Tapering of Chalcogenide Fiber for Mid-infrared Supercontinuum Generation
Published on: May 27, 2013
12.9K
Mid-infrared-to-mid-ultraviolet supercontinuum enhanced by third-to-fifteenth odd harmonics
Optics Letters
|May 1, 2015
Summary
Researchers generated a broad supercontinuum spectrum using a mid-infrared driver, enhancing its high-frequency range with optical harmonics. This technique broadens spectral peaks due to ionization effects, verified by numerical modeling.
Area of Science:
- Nonlinear Optics
- Laser Physics
- Spectroscopy
Background:
- Supercontinuum generation is crucial for various spectroscopic applications.
- Mid-infrared (MIR) drivers offer unique advantages for nonlinear optical processes.
Purpose of the Study:
- To generate a high-energy, broadband supercontinuum using a MIR optical parametric chirped-pulse amplifier (OPCPA).
- To investigate the enhancement of the supercontinuum's high-frequency wing via optical harmonics.
- To analyze the spectral broadening mechanisms, including ionization-induced blueshift.
Main Methods:
- Utilizing a 0.3-TW, 3.9-μm MIR OPCPA as the driver laser.
- Inducing laser filamentation in ambient air for supercontinuum generation.
- Observing and analyzing optical harmonics up to the 15th order.
- Employing numerical modeling to verify spectral broadening mechanisms.
Main Results:
- Generation of a supercontinuum spanning 4.7 octaves (250–6500 nm).
- Enhancement of the supercontinuum's high-frequency wing by odd-order optical harmonics.
- Observation of well-resolved, broadened harmonic peaks attributed to spatially nonuniform ionization-induced blueshift.
Conclusions:
- A high-energy supercontinuum can be effectively generated and controlled using MIR OPCPA drivers.
- Optical harmonic generation plays a significant role in extending the supercontinuum spectrum to higher frequencies.
- Ionization dynamics significantly influence spectral broadening in laser-induced filaments.
Related Concept Videos
Infrared (IR) Spectroscopy: Overview
7.6K
When electromagnetic radiation passes through a material, atoms or molecules transition from a lower to a higher energy state by absorbing radiation corresponding to the energy difference between the two states. The absorption of infrared (IR) radiation causes transitions between vibrational energy levels in a molecule. Therefore, IR spectroscopy is a useful analytical tool for determining the molecular structure of molecules.
Different compounds display unique properties due to their...
Different compounds display unique properties due to their...
7.6K
IR Frequency Region: X–H Stretching
1.8K
In IR spectroscopy, signals produced by the X−H bonds (such as C−H, O−H, or N−H) can be observed in the frequency range of 2700–4000 cm–1. The C−H stretching vibration forms sharp bands in the region 2850–3000 cm–1. The presence of the O−H stretching vibration leads to the forming of an absorption band in the frequency range 3650–3200 cm−1. At the same time, N−H stretching can be confirmed by absorption bands in...
1.8K
IR Spectroscopy: Molecular Vibration Overview
6.5K
When Infrared (IR) radiation passes through a covalently bonded molecule, the bonds transition from lower to higher vibrational levels. The fundamental vibrational motions that result in infrared absorption can be classified as stretching or bending vibrations.
Stretching vibrations are vibrational motions that occur along the bond line, changing the bond length or distance between two bonded atoms. They are further distinguished as symmetric or asymmetric. In symmetric stretching, the...
Stretching vibrations are vibrational motions that occur along the bond line, changing the bond length or distance between two bonded atoms. They are further distinguished as symmetric or asymmetric. In symmetric stretching, the...
6.5K
IR Absorption Frequency: Hybridization
1.7K
Hydrocarbons such as alkanes, alkenes, and alkynes show characteristic C–H stretching absorption bands. These IR stretching frequencies depend on the hybridization of the involved carbon atom and can be explained in terms of the s character of each hybridized atomic orbital.
Among the sp, sp2, and sp3 hybridized orbitals, sp orbitals have the maximum s character (50%). Consequently, the electrons are held more closely to the nucleus, resulting in stronger and shorter C–H bonds that...
Among the sp, sp2, and sp3 hybridized orbitals, sp orbitals have the maximum s character (50%). Consequently, the electrons are held more closely to the nucleus, resulting in stronger and shorter C–H bonds that...
1.7K
Ultraviolet and Visible (UV–Vis) Spectroscopy: Overview
8.7K
Ultraviolet–visible (UV–visible or UV–Vis) spectroscopy is an analytical technique that investigates the interaction between matter and UV–Vis light within the electromagnetic spectrum. This method is widely used for its versatility, simplicity, and relatively quick data acquisition, making it valuable for both qualitative and quantitative analysis. When UV–Vis radiation passes through a material, molecules absorb light depending on the energy required for...
8.7K
IR Spectrum Peak Broadening: Hydrogen Bonding
2.3K
The vibrational frequency of a bond is directly proportional to its bond strength. As a result, stronger bonds vibrate at higher frequencies, while weaker bonds vibrate at lower frequencies. The stretching vibration of the strong O–H bond in alcohols and phenols (very dilute solution or gas phase) appears as a sharp peak at 3600–3650 cm−1.
However, the extent of hydrogen bonding influences the observed stretching frequency and band broadening. Intermolecular or intramolecular...
However, the extent of hydrogen bonding influences the observed stretching frequency and band broadening. Intermolecular or intramolecular...
2.3K

