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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:
Characteristics of Series Resonant Circuit01:24

Characteristics of Series Resonant Circuit

Series resonance occurs in a circuit containing inductive (L), capacitive (C), and resistive (R) elements connected sequentially. At the resonance frequency, the inductive and capacitive reactances are equal in magnitude but opposite in sign, effectively canceling each other. This causes the circuit's impedance is minimal, primarily determined by the resistance R. The resonant frequency of an RLC circuit is defined as:
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
Resonance in an AC Circuit01:26

Resonance in an AC Circuit

The property of an inductor makes it resist any change in the current passing through it, while the property of a capacitor is to build up the charge across its terminals. Hence, if an inductor and capacitor are connected in series, they have opposite effects on the relative phase between current and voltage. The current through the circuit undergoes forced oscillation at the frequency of the source. The resistance term in an R-L-C circuit acts as a damping term because power is dissipated...
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Sound Waves: Resonance01:14

Sound Waves: Resonance

Resonance is produced depending on the boundary conditions imposed on a wave. Resonance can be produced in a string under tension with symmetrical boundary conditions (i.e., has a node at each end). A node is defined as a fixed point where the string does not move. The symmetrical boundary conditions result in some frequencies resonating and producing standing waves, while other frequencies interfere destructively. Sound waves can resonate in a hollow tube, and the frequencies of the sound...

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Related Experiment Video

Updated: Jun 22, 2026

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
07:42

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

Published on: December 15, 2021

Rotating and Fugitive Cavity Solitons in semiconductor microresonators.

R Kheradmand, L Lugiato, G Tissoni

    Optics Express
    |May 28, 2009
    PubMed
    Summary

    We present two methods for controlling cavity soliton motion, enabling all-optical clocking and synchronization. These techniques leverage phase gradients and thermal dynamics for predictable soliton movement, paving the way for advanced optical systems.

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    Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
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    Published on: December 15, 2021

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    10:26

    Fabrication and Characterization of Superconducting Resonators

    Published on: May 21, 2016

    Area of Science:

    • Nonlinear Optics
    • Photonics
    • Optical Communications

    Background:

    • Cavity solitons are localized light structures within optical cavities.
    • Controlling their motion is crucial for applications like all-optical signal processing.
    • Existing methods for soliton control are limited.

    Purpose of the Study:

    • To explore novel methods for controlling cavity soliton motion.
    • To demonstrate periodic motion of cavity solitons for clocking and synchronization.
    • To investigate the influence of thermal dynamics and phase modulations on soliton behavior.

    Main Methods:

    • Exploiting soliton drift in phase gradients using a doughnut-shaped holding beam.
    • Utilizing thermally induced spontaneous motion of solitons.
    • Applying phase and amplitude modulations to the holding beam.
    • Introducing a 2D phase modulation to induce random walk behavior.

    Main Results:

    • Demonstrated rotational motion of cavity solitons along a doughnut beam annulus.
    • Showcased control over thermally induced soliton motion via beam modulations.
    • Observed a 'Fugitive Soliton' exhibiting a random walk, escaping its self-generated thermal minimum.

    Conclusions:

    • Two distinct methods enable controlled periodic motion of cavity solitons.
    • These findings offer pathways for soliton-based all-optical clocking and synchronization.
    • The 'Fugitive Soliton' phenomenon presents new possibilities for soliton dynamics research.