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

Time and frequency -Domain Interpretation of Phase-lead Control01:24

Time and frequency -Domain Interpretation of Phase-lead Control

490
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...
490
Gain01:15

Gain

526
Gain and phase shift are properties of linear circuits that describe the effect a circuit has on a sinusoidal input voltage or current. The circuit's behavior that contains reactive elements will depend on the frequency of the input sinusoid. As a result, it is observed that the gain and phase shift will all be frequency functions.
Gain:
Suppose Vin is the input and Vout is the output signal to a circuit.
526
Time and frequency -Domain Interpretation of Phase-lag Control01:21

Time and frequency -Domain Interpretation of Phase-lag Control

429
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...
429
Graphical and Analytic Representation of Sinusoids01:20

Graphical and Analytic Representation of Sinusoids

1.1K
Analyzing two sinusoidal voltages with equal amplitude and period but different phases on an oscilloscope, an instrument used to display and analyze waveforms, involves a three-step process.
The first step is measuring the peak-to-peak value, which is twice the amplitude of the sinusoid. This provides information about the maximum voltage swing of the waveform.
Secondly, the period and angular frequency are determined. The period is the time taken for one complete cycle of the waveform, while...
1.1K
Frequency Response of a Circuit01:20

Frequency Response of a Circuit

897
Inductive circuits present intriguing challenges in electrical engineering, particularly during the transition from the time domain to the frequency domain. This transformation involves converting inductors into impedances and utilizing phasor representation.
The transfer function is pivotal in characterizing how these circuits react to various frequencies, facilitating a profound understanding of their behavior. An essential parameter is the time constant, signifying the...
897
Interference: Path Lengths01:10

Interference: Path Lengths

2.3K
Consider two sources of sound, that may or may not be in phase, emitting waves at a single frequency, and consider the frequencies to be the same.
Two special sources may be considered when they are in phase. This can be easily achieved by feeding the two sources from the same source. An example would be synchronizing the two speakers by feeding them with the same source, such as the sound waves produced by a tuning fork. This setup ensures that the two sources have the same frequency and are...
2.3K

You might also read

Related Articles

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

Sort by
Same author

Valley-Dependent Emission Patterns Enabled by Plasmonic Nanoantennas.

ACS nano·2026
Same author

Enhanced Photon-Pair Generation from a van der Waals Metasurface.

Nano letters·2025
Same author

Nonlinearity symmetry breaking for generating tunable quantum entanglement in semiconductor metasurfaces.

Science advances·2025
Same author

Metasurface-enabled small-satellite polarisation imaging.

Nanoscale advances·2025
Same author

Integrated generation of vortices and frequency conversion with metasurfaces.

Light, science & applications·2025
Same author

Inverse design of nonlinear metasurfaces for sum frequency generation.

Nanophotonics (Berlin, Germany)·2024

Related Experiment Video

Updated: Mar 2, 2026

Shaping the Amplitude and Phase of Laser Beams by Using a Phase-only Spatial Light Modulator
08:39

Shaping the Amplitude and Phase of Laser Beams by Using a Phase-only Spatial Light Modulator

Published on: January 28, 2019

10.4K

Non-reciprocal geometric phase in nonlinear frequency conversion.

Kai Wang, Yu Shi, Alexander S Solntsev

    Optics Letters
    |May 16, 2017
    PubMed
    Summary
    This summary is machine-generated.

    Researchers have developed a non-reciprocal geometric phase for nonlinear frequency conversion, overcoming limitations of existing devices. This robust and practical method offers controllable phase properties using a single waveguide and pump.

    More Related Videos

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

    Generation and Coherent Control of Pulsed Quantum Frequency Combs

    Published on: June 8, 2018

    9.8K
    The Frequency Domain Thermoreflectance Technique for Thermal Property Measurements
    09:10

    The Frequency Domain Thermoreflectance Technique for Thermal Property Measurements

    Published on: December 5, 2025

    971

    Related Experiment Videos

    Last Updated: Mar 2, 2026

    Shaping the Amplitude and Phase of Laser Beams by Using a Phase-only Spatial Light Modulator
    08:39

    Shaping the Amplitude and Phase of Laser Beams by Using a Phase-only Spatial Light Modulator

    Published on: January 28, 2019

    10.4K
    Generation and Coherent Control of Pulsed Quantum Frequency Combs
    06:42

    Generation and Coherent Control of Pulsed Quantum Frequency Combs

    Published on: June 8, 2018

    9.8K
    The Frequency Domain Thermoreflectance Technique for Thermal Property Measurements
    09:10

    The Frequency Domain Thermoreflectance Technique for Thermal Property Measurements

    Published on: December 5, 2025

    971

    Area of Science:

    • Photonics
    • Nonlinear Optics
    • Quantum Optics

    Background:

    • Geometric phase in nonlinear frequency conversion is crucial for optical device performance.
    • Existing devices often face limitations due to dynamic reciprocity.
    • Achieving non-reciprocity is key to overcoming these limitations.

    Purpose of the Study:

    • To analytically and numerically describe the geometric phase in nonlinear frequency conversion.
    • To demonstrate a method for achieving non-reciprocal geometric phase.
    • To propose a practical implementation for non-reciprocal photonic devices.

    Main Methods:

    • Analytical description of geometric phase.
    • Numerical simulations of nonlinear frequency conversion.
    • Investigation of momentum-dependent photonic transitions.

    Main Results:

    • The geometric phase can be made non-reciprocal through momentum-dependent photonic transitions.
    • This non-reciprocity circumvents issues associated with dynamic reciprocity in Kerr devices.
    • A practical implementation using a single waveguide and pump is proposed.

    Conclusions:

    • The proposed method offers a robust and controllable way to achieve non-reciprocal geometric phase.
    • This approach promises improved performance and reliability in photonic devices.
    • Controllability via pump and robustness against fabrication errors are key advantages.