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Related Concept Videos

IR Spectrometers01:25

IR Spectrometers

There are two main infrared (IR) spectrophotometers: dispersive IR spectrometers and Fourier transform infrared (FTIR) spectrometers. In a dispersive IR spectrometer, a beam of infrared radiation produced by a hot wire is divided into two parallel equal-intensity beams using mirrors. One beam passes through the sample, while another is a reference beam. The beams then move through the monochromator, which separates the radiations into a continuous spectrum of different frequencies. The...
Time and frequency -Domain Interpretation of Phase-lag Control01:21

Time and frequency -Domain Interpretation of Phase-lag Control

Phase-lag controllers are widely used in control systems to improve stability and reduce steady-state errors. A dimmer switch controlling the brightness of a light bulb serves as a practical example of phase-lag control, gradually adjusting the bulb's brightness. Mathematically, phase-lag control or low-pass filtering is represented when the factor 'a' is less than 1.
Phase-lag controllers do not place a pole at zero, but instead influence the steady-state error by amplifying any finite,...
Time and frequency -Domain Interpretation of Phase-lead Control01:24

Time and frequency -Domain Interpretation of Phase-lead Control

Phase-lead controllers are commonly used in various control systems to enhance response speed and stability. Adjusting the brightness on a television screen offers a practical example of phase-lead control. When contrast is enhanced, a phase-lead controller is employed. Mathematically, phase-lead control is identified when the first parameter is smaller than the second.
The design of phase-lead control involves the strategic placement of poles and zeros to balance steady-state error and system...
Discrete Fourier Transform01:15

Discrete Fourier Transform

The Discrete Fourier Transform (DFT) is a fundamental tool in signal processing, extending the discrete-time Fourier transform by evaluating discrete signals at uniformly spaced frequency intervals. This transformation converts a finite sequence of time-domain samples into frequency components, each representing complex sinusoids ordered by frequency. The DFT translates these sequences into the frequency domain, effectively indicating the magnitude and phase of each frequency component present...
IR Frequency Region: Fingerprint Region01:03

IR Frequency Region: Fingerprint Region

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 C=O, C=N, and C=C occur between 1600–1850 cm−1.
The...
Discrete-time Fourier transform01:26

Discrete-time Fourier transform

The Discrete-Time Fourier Transform (DTFT) is an essential mathematical tool for analyzing discrete-time signals, converting them from the time domain to the frequency domain. This transformation allows for examining the frequency components of discrete signals, providing insights into their spectral characteristics. In the DTFT, the continuous integral used in the continuous-time Fourier transform is replaced by a summation to accommodate the discrete nature of the signal.
One of the notable...

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A Multimodal Wide-Field Fourier-Transform Raman Microscope
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Frequency-domain interferometer for femtosecond time-resolved phase spectroscopy.

E Tokunaga, A Terasaki, T Kobayashi

    Optics Letters
    |October 2, 2009
    PubMed
    Summary

    A novel femtosecond interferometer reveals transient oscillations in difference phase spectra (DPS). This breakthrough provides direct evidence of induced phase modulation in absorptive materials.

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    Area of Science:

    • Ultrafast Spectroscopy
    • Nonlinear Optics
    • Materials Science

    Background:

    • Understanding light-matter interactions at ultrafast timescales is crucial for developing advanced optical materials and devices.
    • Previous methods lacked the simultaneous resolution of both phase and transmission changes in ultrafast spectroscopy.
    • Absorptive materials exhibit complex dynamic responses to intense light pulses, necessitating advanced characterization techniques.

    Purpose of the Study:

    • To develop a new femtosecond time-resolved interferometer for simultaneous measurement of difference phase spectra (DPS) and difference transmission spectra.
    • To investigate transient phenomena and spectral dynamics in absorptive materials following ultrafast optical excitation.
    • To provide direct evidence for induced phase modulation in absorptive materials.

    Main Methods:

    • Development of a novel femtosecond time-resolved interferometer utilizing frequency-domain interference fringes.
    • Simultaneous acquisition of DPS and difference transmission spectra using a multichannel spectrometer.
    • Time-resolved observation of spectral shifts and transient oscillations in the DPS.

    Main Results:

    • Successfully developed and implemented a femtosecond time-resolved interferometer.
    • Observed transient oscillations in DPS for the first time.
    • Time-resolved spectral shift of the probe pulse correlated with the rise in DPS, confirming induced phase modulation.

    Conclusions:

    • The developed interferometer enables simultaneous, high-resolution measurement of ultrafast phase and transmission dynamics.
    • Transient oscillations in DPS are a clear indicator of induced phase modulation in absorptive materials.
    • This technique opens new avenues for studying ultrafast nonlinear optical phenomena in various materials.