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Related Concept Videos

Cascaded Op Amps01:16

Cascaded Op Amps

Operational amplifiers (op-amps) are versatile electronic components that can be interconnected in a cascade - one after another in a linear sequence. This cascading is possible due to their infinite input resistance and zero output resistance, allowing them to maintain their input-output relationships even when connected in series.
In a cascaded system, each op-amp is referred to as a stage. The output of one stage drives the input of the subsequent stage. As the input signal passes through...
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
Damped Oscillations01:07

Damped Oscillations

In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Forced Oscillations01:06

Forced Oscillations

When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
Propagation of Waves01:07

Propagation of Waves

When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:

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Related Experiment Video

Updated: Jun 23, 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

Cascaded optical parametric oscillations.

M Vaidyanathan, R Eckardt, V Dominic

    Optics Express
    |April 18, 2009
    PubMed
    Summary
    This summary is machine-generated.

    Researchers studied a tunable optical parametric oscillator (OPO) using lithium niobate. They observed an efficient secondary OPO and found theoretical predictions matched experimental results, offering insights into pulsed parametric oscillation dynamics.

    Related Experiment Videos

    Last Updated: Jun 23, 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

    Area of Science:

    • Nonlinear optics
    • Quantum optics

    Background:

    • Optical parametric oscillators (OPOs) are crucial for generating tunable laser light.
    • Periodically poled lithium niobate (PPLN) is a key material for nonlinear optical frequency conversion.

    Purpose of the Study:

    • To investigate the spectral and temporal characteristics of a 1.064-mm pumped optical parametric oscillator.
    • To analyze the behavior of a secondary OPO generated within the primary OPO system.
    • To validate theoretical models against experimental observations of pulsed parametric oscillation.

    Main Methods:

    • Utilized a continuously tunable optical parametric oscillator (OPO) system.
    • Employed a periodically poled lithium niobate nonlinear crystal.
    • Observed and characterized spectral and temporal properties of the generated optical signals.

    Main Results:

    • Successfully observed the spectral and temporal characteristics of the 1.064-mm pumped OPO.
    • Demonstrated an efficient secondary OPO, pumped by the resonant signal of the primary OPO.
    • Achieved agreement between theoretical predictions and experimental observations.

    Conclusions:

    • The study provides valuable insights into the dynamics of pulsed parametric oscillation.
    • The observed secondary OPO highlights efficient nonlinear frequency conversion possibilities.
    • Validated theoretical models enhance the understanding and design of OPO systems.