Related Experiment Video
Updated: Aug 8, 2025

10:17
20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier
Published on: July 12, 2017
11.6K
Transition to hyperchaos and rare large-intensity pulses in Zeeman laser
S Leo Kingston1, Marek Balcerzak1, Syamal K Dana1
1Division of Dynamics, Lodz University of Technology, 90-924 Lodz, Poland.
Chaos (Woodbury, N.Y.)
|March 1, 2023
Summary
A discontinuous transition to hyperchaos was observed in the Zeeman laser model. This phenomenon, characterized by extreme intensity pulses, is robust to noise and common in low-dimensional systems.
Area of Science:
- Nonlinear dynamics
- Laser physics
- Chaos theory
Background:
- Nonlinear systems often exhibit complex dynamics, including chaos.
- Understanding transitions to more complex states like hyperchaos is crucial.
- Previous studies recognized extreme events in chaotic systems but lacked specific classification.
Purpose of the Study:
- To investigate the transition to hyperchaos in the Zeeman laser model.
- To analyze the characteristics of extreme intensity pulses during this transition.
- To explore the robustness of hyperchaos to noise and its prevalence in low-dimensional systems.
Main Methods:
- Analysis of the Zeeman laser model across different nonlinear instability routes.
- Identification of critical parameters for the onset of hyperchaos.
- Characterization of large-intensity pulses and system attractor behavior.
- Investigation of noise effects on the transition and critical parameters.
Main Results:
- A discontinuous transition to hyperchaos was observed at discrete critical parameters for three instability types.
- Hyperchaos onset coincided with sudden attractor expansion and recurrent large-intensity pulses.
- Pomeau-Manneville intermittency showed hysteresis, unlike other routes.
- The phenomenon is robust to weak noise, with noise shifting the transition parameter.
Conclusions:
- The Zeeman laser model exhibits a distinct transition to hyperchaos, generating extreme events.
- These extreme events, while robust to noise, may require new metrics for classification beyond standard chaos.
- The findings highlight the commonality of such dynamics in low-dimensional systems and the need for refined analytical tools.
Related Concept Videos
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences
870
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.
870
Atomic Nuclei: Nuclear Relaxation Processes
696
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
696
Atomic Nuclei: Larmor Precession Frequency
1.6K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
1.6K

