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Related Concept Videos

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...
Propagation Speed of Electromagnetic Waves01:30

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Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
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.
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Generating Electromagnetic Radiations01:10

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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 the...
Oscillations In An LC Circuit01:30

Oscillations In An LC Circuit

An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by

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Related Experiment Video

Updated: Jul 9, 2026

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
09:23

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators

Published on: May 30, 2014

Broadband optical frequency comb generation with a phase-modulated parametric oscillator.

S A Diddams, L S Ma, J Ye

    Optics Letters
    |December 15, 2007
    PubMed
    Summary

    We developed a new broadband optical frequency comb generator using a parametric oscillator and phase modulator. This device creates a wide 20 nm comb spanning 5.3 THz with high signal-to-noise ratio.

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    Published on: February 6, 2014

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    Last Updated: Jul 9, 2026

    Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
    09:23

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    Published on: May 30, 2014

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

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    Published on: June 8, 2018

    Quasi-light Storage for Optical Data Packets
    07:45

    Quasi-light Storage for Optical Data Packets

    Published on: February 6, 2014

    Area of Science:

    • Photonics and Laser Technology
    • Nonlinear Optics

    Background:

    • Optical frequency combs are crucial for precision measurements.
    • Generating broadband combs often requires complex setups.

    Purpose of the Study:

    • To introduce a novel, compact broadband optical frequency comb generator.
    • To demonstrate a comb spanning over 20 nm using a parametric oscillator.

    Main Methods:

    • Utilized a parametric oscillator pumped by 532-nm light.
    • Incorporated an intracavity electro-optic phase modulator.
    • Leveraged mode coupling to achieve broadband generation.

    Main Results:

    • Generated a dispersion-limited optical frequency comb spanning 20 nm (5.3 THz).
    • Observed a signal-to-noise ratio exceeding 30 dB in a 300-kHz bandwidth.
    • The comb structure was generated around both signal and idler fields.

    Conclusions:

    • The proposed device offers a novel approach to broadband optical frequency comb generation.
    • The system demonstrates potential for applications requiring wide spectral coverage and high precision.