Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Intensity Of Electromagnetic Waves01:22

Intensity Of Electromagnetic Waves

5.6K
The energy transport per unit area per unit time, or the Poynting vector, gives the energy flux of an electromagnetic wave at any specific time. For a plane electromagnetic wave with E0 and B0 as the peak electric and magnetic fields and traveling along the x-axis, the time-varying energy flux can be given by the following equation:
5.6K
IR Frequency Region: Fingerprint Region01:03

IR Frequency Region: Fingerprint Region

1.8K
IR spectra are divided into two main regions: the diagnostic region and the fingerprint region. The diagnostic region of the spectrum lies above 1500 cm−1. The absorptions resulting from single-bond vibrations of the N–H, C–H, and O–H stretch at higher wavenumbers and appear on the left side of the spectrum. The stretching absorptions of the C≡C and C≡N occur between 2100–2300 cm−1. In contrast, those arising from stretching absorptions of the...
1.8K
IR Frequency Region: X–H Stretching01:24

IR Frequency Region: X–H Stretching

1.3K
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...
1.3K
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

1.6K
A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
1.6K
Difference from Background: Limit of Detection01:05

Difference from Background: Limit of Detection

8.0K
The limit of detection (LOD) is the smallest amount of analyte that can be distinguished from the background noise. The LOD value corresponds to the concentration at which the analyte signal is three times larger than the standard deviation of the blank signal. Below this value, the analyte signal cannot be differentiated from the background noise. It is calculated by dividing the calibration slope by 3 times the standard deviation of the blank signals.
The LOD indicates the presence or absence...
8.0K
IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations01:08

IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations

1.6K
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...
1.6K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Optical frequency comb double-resonance spectroscopy of the 9030-9175 cm-1 states of ethylene.

The Journal of chemical physics·2026
Same author

Overview of Systematic Monitoring Networks for Surface Water Quality in the Amazon River Basin.

Environmental management·2026
Same author

Redirection and reshaping of intense extreme-ultraviolet radiation.

Science advances·2026
Same author

Combined frequency comb and continuous wave cavity-enhanced optical-optical double-resonance spectrometer in the 1.7 µm range.

Optics express·2025
Same author

Improved temporal characteristics for post-compressed pulses via application-tailored nonlinear polarization ellipse rotation.

Optics letters·2024
Same author

Measurement and assignment of J = 5 to 9 rotational energy levels in the 9070-9370 cm-1 range of methane using optical frequency comb double-resonance spectroscopy.

The Journal of chemical physics·2024

Related Experiment Video

Updated: Dec 25, 2025

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

9.6K

Intensity noise optimization of a mid-infrared frequency comb difference-frequency generation source.

Vinicius Silva de Oliveira, Axel Ruehl, Piotr Masłowski

    Optics Letters
    |April 3, 2020
    PubMed
    Summary

    Optimizing temporal overlap in mid-infrared frequency comb sources minimizes relative intensity noise (RIN). Active stabilization of pump-signal pulse delay enhances signal-to-noise ratio for absorption spectra.

    More Related Videos

    Quasi-light Storage for Optical Data Packets
    07:45

    Quasi-light Storage for Optical Data Packets

    Published on: February 6, 2014

    11.2K
    Infrared Degenerate Four-wave Mixing with Upconversion Detection for Quantitative Gas Sensing
    10:42

    Infrared Degenerate Four-wave Mixing with Upconversion Detection for Quantitative Gas Sensing

    Published on: March 22, 2019

    6.5K

    Related Experiment Videos

    Last Updated: Dec 25, 2025

    Generation and Coherent Control of Pulsed Quantum Frequency Combs
    06:42

    Generation and Coherent Control of Pulsed Quantum Frequency Combs

    Published on: June 8, 2018

    9.6K
    Quasi-light Storage for Optical Data Packets
    07:45

    Quasi-light Storage for Optical Data Packets

    Published on: February 6, 2014

    11.2K
    Infrared Degenerate Four-wave Mixing with Upconversion Detection for Quantitative Gas Sensing
    10:42

    Infrared Degenerate Four-wave Mixing with Upconversion Detection for Quantitative Gas Sensing

    Published on: March 22, 2019

    6.5K

    Area of Science:

    • Nonlinear Optics
    • Spectroscopy
    • Frequency Comb Technology

    Background:

    • Mid-infrared (MIR) frequency combs are crucial for high-resolution spectroscopy.
    • Relative intensity noise (RIN) in the idler pulse impacts spectral measurement sensitivity.
    • Precise control over pump and signal pulse interactions is vital for noise reduction.

    Purpose of the Study:

    • To experimentally investigate the impact of temporal overlap between pump and signal pulses on the idler pulse's RIN.
    • To demonstrate active stabilization of the MIR frequency comb to minimize RIN and improve spectral quality.

    Main Methods:

    • Utilizing a difference-frequency generation (DFG) based MIR frequency comb source.
    • Scanning the temporal delay between 130 fs pump and signal pulses to measure RIN.
    • Implementing an online RIN detector and feedback control for active stabilization of pulse delay.

    Main Results:

    • A minimum RIN was observed with a 20 fs delay width.
    • A 20 dB increase in RIN was measured at the edges of the optimal delay.
    • Active stabilization successfully reduced RIN and enhanced the signal-to-noise ratio (SNR) of MIR absorption spectra.

    Conclusions:

    • Temporal overlap of pump and signal pulses significantly affects MIR frequency comb RIN.
    • Active stabilization of pulse delay is an effective method for noise reduction.
    • Improved SNR through active stabilization enables more sensitive MIR spectroscopic measurements.