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

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
MOSFET: Enhancement Mode01:22

MOSFET: Enhancement Mode

Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no current...
Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
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

You might also read

Related Articles

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

Sort by
Same author

Signature of glassy dynamics in dynamic mode decompositions.

Physical review. E·2026
Same author

Erratum: Sub-50-femtosecond gain-managed amplified pulses enhance nonlinear ablation efficiency: publisher's note.

Biomedical optics express·2026
Same author

Reservoir computing for system identification and model predictive control.

Neural networks : the official journal of the International Neural Network Society·2026
Same author

Single-mode nonlinear amplification of femtosecond pulses in a multimode-fiber regenerative amplifier.

Optics letters·2026
Same author

Learning the bistable cortical dynamics of the sleep-onset period.

PLoS computational biology·2026
Same author

Sparse identification of nonlinear dynamics and Koopman operators with Shallow Recurrent Decoder Networks.

Proceedings of the National Academy of Sciences of the United States of America·2026

Related Experiment Video

Updated: Jun 17, 2026

Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements
14:18

Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements

Published on: February 28, 2016

Transition dynamics for multi-pulsing in mode-locked lasers.

Brandon G Bale1, Khanh Kieu, J Nathan Kutz

  • 1Photonics Research Group, School of Engineering and Applied Science, Aston University, Birmingham B4 7ET, UK. b.bale@aston.ac.uk

Optics Express
|January 7, 2010
PubMed
Summary

Researchers studied laser systems transitioning to multi-pulse modelocking. They found a universal chaotic behavior emerges near this transition, characterized by Hopf bifurcations and oscillatory modes.

More Related Videos

Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy
08:48

Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy

Published on: November 22, 2019

Direct Imaging of Laser-driven Ultrafast Molecular Rotation
10:52

Direct Imaging of Laser-driven Ultrafast Molecular Rotation

Published on: February 4, 2017

Related Experiment Videos

Last Updated: Jun 17, 2026

Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements
14:18

Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements

Published on: February 28, 2016

Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy
08:48

Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy

Published on: November 22, 2019

Direct Imaging of Laser-driven Ultrafast Molecular Rotation
10:52

Direct Imaging of Laser-driven Ultrafast Molecular Rotation

Published on: February 4, 2017

Area of Science:

  • Laser Physics
  • Nonlinear Dynamics
  • Optical Engineering

Background:

  • Mode-locked lasers are crucial for various scientific and technological applications.
  • Understanding the transition to multi-pulse operation is key to controlling laser output.
  • Previous studies have not fully characterized the dynamics near the N to N+1 pulse transition.

Purpose of the Study:

  • To experimentally and theoretically investigate the parameter space near the transition to multi-pulse modelocking.
  • To characterize the onset of instability and the resulting chaotic behavior.
  • To establish the universality of this phenomenon in mode-locked lasers.

Main Methods:

  • Refined tuning of the gain pump level in a laser system.
  • Experimental observation of laser dynamics near the multi-pulse transition.
  • Theoretical modeling of the system's behavior, focusing on Hopf bifurcations and oscillatory modes.

Main Results:

  • Identified a Hopf (periodic) bifurcation initiating instability near the transition.
  • Observed chaotic behavior between single- and multi-pulse operation as cavity energy increased.
  • Demonstrated good qualitative agreement between theoretical predictions and experimental results.

Conclusions:

  • The transition to multi-pulsing in mode-locked lasers exhibits universal characteristics.
  • Hopf bifurcations and chaotic dynamics play a significant role in this transition.
  • This study provides the first comprehensive theoretical and experimental characterization of this phenomenon.