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

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:
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...
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...
Concept of Resonance and its Characteristics01:19

Concept of Resonance and its Characteristics

If a driven oscillator needs to resonate at a specific frequency, then very light damping is required. An example of light damping includes playing piano strings and many other musical instruments. Conversely, to achieve small-amplitude oscillations as in a car's suspension system, heavy damping is required. Heavy damping reduces the amplitude, but the tradeoff is that the system responds at more frequencies. Speed bumps and gravel roads prove that even a car's suspension system is not immune...
The de Broglie Wavelength02:32

The de Broglie Wavelength

In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
Parallel Resonance01:23

Parallel Resonance

The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:

You might also read

Related Articles

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

Sort by
Same author

Integrated O- and C-band silicon-lithium niobate Mach-Zehnder modulators with 100 GHz bandwidth, low voltage, and low loss.

Optics express·2023
Same author

110 GHz, 110 mW hybrid silicon-lithium niobate Mach-Zehnder modulator.

Scientific reports·2022
Same author

High-speed silicon microresonator modulators with high optical modulation amplitude (OMA) at input powers >10 mW.

Optics express·2022
Same author

Consequences of quantum noise control for the relaxation resonance frequency and phase noise in heterogeneous Silicon/III-V lasers.

Scientific reports·2022
Same author

Quantum Wave-Particle Duality in Free-Electron-Bound-Electron Interaction.

Physical review letters·2021
Same author

Gover and Yariv Reply.

Physical review letters·2021

Related Experiment Video

Updated: Jul 10, 2026

Microwave Photonics Systems Based on Whispering-gallery-mode Resonators
12:18

Microwave Photonics Systems Based on Whispering-gallery-mode Resonators

Published on: August 5, 2013

Nonlinear dispersion in a coupled-resonator optical waveguide.

Shayan Mookherjea, Donald S Cohen, Amnon Yariv

    Optics Letters
    |November 21, 2007
    PubMed
    Summary
    This summary is machine-generated.

    This study presents a nonperturbative method for calculating optical pulse propagation in coupled-resonator optical waveguides. It identifies conditions to minimize pulse distortion, crucial for waveguide design.

    More Related Videos

    Fabrication And Characterization Of Photonic Crystal Slow Light Waveguides And Cavities
    11:08

    Fabrication And Characterization Of Photonic Crystal Slow Light Waveguides And Cavities

    Published on: November 30, 2012

    Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
    12:19

    Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source

    Published on: April 4, 2017

    Related Experiment Videos

    Last Updated: Jul 10, 2026

    Microwave Photonics Systems Based on Whispering-gallery-mode Resonators
    12:18

    Microwave Photonics Systems Based on Whispering-gallery-mode Resonators

    Published on: August 5, 2013

    Fabrication And Characterization Of Photonic Crystal Slow Light Waveguides And Cavities
    11:08

    Fabrication And Characterization Of Photonic Crystal Slow Light Waveguides And Cavities

    Published on: November 30, 2012

    Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
    12:19

    Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source

    Published on: April 4, 2017

    Area of Science:

    • Photonics and Waveguide Optics
    • Condensed Matter Physics

    Background:

    • Coupled-resonator optical waveguides (CROWs) are key components in integrated photonics.
    • Understanding optical pulse propagation in CROWs is essential for device performance.
    • Dispersion effects significantly impact pulse behavior in waveguides.

    Purpose of the Study:

    • To develop a nonperturbative calculation method for optical pulse propagation in CROWs.
    • To analyze the influence of nonlinear dispersion on pulse dynamics.
    • To identify design parameters that minimize pulse distortion in CROWs.

    Main Methods:

    • Utilized the conventional tight-binding approximation.
    • Developed a nonperturbative calculation framework applicable to all orders of dispersion.
    • Analyzed the nonlinear dispersion relationship within the CROW system.

    Main Results:

    • Successfully calculated optical pulse propagation nonperturbatively, accounting for all dispersion orders.
    • Identified critical physical parameter limits and approximations for minimizing pulse distortion.
    • Demonstrated the framework's validity even with a nonlinear dispersion relationship.

    Conclusions:

    • The developed nonperturbative method provides accurate predictions for pulse propagation in CROWs.
    • Understanding parameter limits is fundamental for designing distortion-free optical waveguides.
    • The tight-binding approximation framework offers broad applicability in optical and condensed matter systems.