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

Small-Signal Analysis of MOSFET Amplifiers01:23

Small-Signal Analysis of MOSFET Amplifiers

786
In small-signal analysis, a MOSFET transistor amplifier acts as a linear amplifier when operating in its saturation region. The gate-to-source voltage (VGS) of the MOSFET is the sum of the DC biasing voltage and the small time-varying input signal. This combination sets up the operating point and modulates the drain current (ID) that flows from the drain to the source. When a small AC signal is superimposed on the DC bias voltage at the gate, the instantaneous drain current comprises three...
786
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

367
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...
367

You might also read

Related Articles

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

Sort by
Same author

Generation of pulses with variable multi-GHz repetition rate in a SOA-based fiber laser with gain instability.

Optics express·2025
Same author

Trainable dynamical masking for readout-free optical computing.

Optics letters·2025
Same author

SOA-based reservoir computing using upsampling.

Optics letters·2024
Same author

Fiber Bragg grating inscription assisted by a spatial light modulator.

Optics letters·2024
Same author

Nonlinear Optical Pulses in Media with Asymmetric Gain.

Physical review letters·2023
Same author

Nonlinear beam tapering and two-dimensional ring solitons.

Physical review. E·2022
Same journal

Gaussian-modulated continuous-variable quantum key distribution over 60 km fiber using an integrated silicon photonic receiver.

Optics letters·2026
Same journal

E2E-OCT: end-to-end joint learning model using optical coherence tomography images for vocal cord leukoplakia diagnosis.

Optics letters·2026
Same journal

Holographic generation of panoramic 3D scenes by concave ellipsoidal mirror reflection.

Optics letters·2026
Same journal

Dual-pilot phase recovery with pair-wise maximum-ratio combining for coherent PONs.

Optics letters·2026
Same journal

Mapping the whispering gallery modes of a CaF<sub>2</sub> disk resonator with half-tapered fibers to estimate the fundamental mode volume.

Optics letters·2026
Same journal

Quantitative estimation of deep-subwavelength scale via dark-field scattering axial energy concentration decay profiles.

Optics letters·2026
See all related articles

Related Experiment Video

Updated: Oct 18, 2025

20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier
10:17

20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier

Published on: July 12, 2017

11.7K

Nonlinear spectral blueshift in semiconductor optical amplifiers.

A E Bednyakova, D Khudozhitkova, A Kokhanovskiy

    Optics Letters
    |October 1, 2021
    PubMed
    Summary
    This summary is machine-generated.

    Negatively chirped optical pulses experience a blueshift after amplification in semiconductor optical amplifiers. This wavelength shift can reach 20 nm, impacting optical communications and spectroscopy.

    More Related Videos

    Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
    15:58

    Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing

    Published on: December 3, 2013

    5.9K
    High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
    10:40

    High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

    Published on: June 28, 2016

    7.7K

    Related Experiment Videos

    Last Updated: Oct 18, 2025

    20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier
    10:17

    20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier

    Published on: July 12, 2017

    11.7K
    Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
    15:58

    Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing

    Published on: December 3, 2013

    5.9K
    High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
    10:40

    High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

    Published on: June 28, 2016

    7.7K

    Area of Science:

    • Optics and Photonics
    • Semiconductor Physics

    Background:

    • Semiconductor optical amplifiers (SOAs) are crucial for optical signal amplification.
    • Understanding pulse dynamics within SOAs is essential for advanced optical systems.

    Purpose of the Study:

    • To investigate the spectral peak power shift of negatively chirped optical pulses after amplification.
    • To quantify the blueshift effect in optical pulses propagated through single-mode fiber and SOAs.

    Main Methods:

    • Experimental demonstration of pulse amplification using a semiconductor optical amplifier.
    • Propagation of negatively chirped optical pulses through single-mode fiber.
    • Spectral analysis of optical pulses before and after amplification.

    Main Results:

    • Observed a significant blueshift in the spectral peak power of negatively chirped optical pulses.
    • Demonstrated a central wavelength translation of over 20 nm towards shorter wavelengths.
    • Quantified a 5 THz blueshift for a 1 ps chirped Gaussian pulse (C=-20).

    Conclusions:

    • Semiconductor optical amplifiers can induce a blueshift in negatively chirped optical pulses.
    • The observed blueshift has implications for wavelength control in optical communication systems.
    • This phenomenon offers potential for manipulating optical pulse spectra in fiber-optic applications.