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Related Concept Videos

IR Frequency Region: X–H Stretching01:24

IR Frequency Region: X–H Stretching

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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...
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IR Absorption Frequency: Hybridization01:21

IR Absorption Frequency: Hybridization

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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...
1.5K
IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations01:08

IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations

2.0K
Identical bonds within a polyatomic group can stretch symmetrically (in-phase) or asymmetrically (out-of-phase). Similar to hydrogen bonding, these vibrations also influence the shape of the IR peak. Generally, asymmetric stretching frequencies are higher than symmetric stretching frequencies. For example, primary amines exhibit two distinct IR peaks between 3300–3500 cm−1 corresponding to the symmetric and asymmetric N-H stretching, while secondary amines exhibit a single...
2.0K
IR Frequency Region: Alkene and Carbonyl Stretching01:29

IR Frequency Region: Alkene and Carbonyl Stretching

1.5K
Double bonds in alkenes and carbonyl compounds exhibit stretching frequencies in the diagnostic region of the IR spectrum. In addition, alkenes exhibit vinylic C–H stretching and C–H out-of-plane bending absorptions that are useful for identifying substitution patterns.
Stretching frequencies are affected by several factors, such as resonance, inductive effects, ring strain, dipole moment, and hydrogen bonding. Consequently, the stretching frequency of the carbonyl double bond...
1.5K
Generating Electromagnetic Radiations01:10

Generating Electromagnetic Radiations

8.7K
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in...
8.7K
IR Spectroscopy: Molecular Vibration Overview01:24

IR Spectroscopy: Molecular Vibration Overview

5.8K
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...
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Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Octave-spanning coherent mid-IR generation via adiabatic difference frequency conversion.

Haim Suchowski, Peter R Krogen, Shu-Wei Huang

    Optics Express
    |February 12, 2014
    PubMed
    Summary
    This summary is machine-generated.

    We achieved efficient downconversion of near-infrared pulses to mid-infrared using a novel chirped quasi-phase-matching grating. This method generates broadband mid-IR light, useful for various laser systems.

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    Area of Science:

    • Nonlinear optics
    • Laser physics
    • Materials science

    Background:

    • Broadband mid-infrared (mid-IR) light sources are crucial for spectroscopy and sensing.
    • Existing methods for mid-IR generation often involve complex setups or limited bandwidth.

    Purpose of the Study:

    • To demonstrate efficient downconversion of near-IR pulses to broadband mid-IR pulses.
    • To utilize a single nonlinear and adiabatic chirped quasi-phase-matching grating for this conversion.

    Main Methods:

    • Employed a magnesium oxide doped lithium niobate crystal with a chirped quasi-phase-matching grating.
    • Mixed μJ-energy optical parametric chirped pulse amplifier (OPCPA) pulses (680-870 nm) with a narrowband 1047-nm pulse.

    Main Results:

    • Achieved 1.1-octave-spanning mid-IR pulses from 2 to 5 μm (at -10 dB).
    • Demonstrated near full photon number conversion.
    • Confirmed robustness for various input OPCPA pulses.

    Conclusions:

    • The demonstrated method offers an efficient and robust way to generate broadband mid-IR pulses.
    • This technique is suitable for post-amplification conversion, broadening applicability for near-IR laser systems.