Related Experiment Video
Updated: Aug 6, 2026

14:18
Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements
Published on: February 28, 2016
Intrinsic localized modes and chaos in damped driven rotator lattices
1Department of Physics and Astronomy, Arizona State University, Tempe, Arizona 85287-1504, USA.
Summary
Intrinsic localized rotational modes (ILRMs) in coupled dipole rotator lattices can become chaotic while remaining localized. This study explores generating random arrays of driven ILRMs using chaotic states, revealing unique absorption properties.
Area of Science:
- Nonlinear dynamics
- Condensed matter physics
- Statistical mechanics
Background:
- Coupled classical dipole rotator lattices exhibit complex behaviors.
- Intrinsic localized modes (ILMs) are important nonlinear phenomena.
- Parametric driving and damping introduce rich dynamics.
Purpose of the Study:
- Investigate the onset of chaos in intrinsic localized rotational modes (ILRMs).
- Analyze the stability of chaotic ILRMs.
- Develop a method for generating stationary, randomly spaced arrays of driven ILRMs.
Main Methods:
- Nonlinear stability analysis.
- Numerical simulations of coupled dipole rotator lattices.
- Exploitation of spatially extended chaotic states.
Main Results:
- ILRMs can become chaotic without losing their localized nature.
- A robust scheme for generating randomly spaced driven ILRM arrays was demonstrated.
- The absorption associated with these arrays shows unusual signatures.
Conclusions:
- Chaotic behavior in localized modes is possible and controllable.
- The developed scheme offers a novel way to create ordered structures from chaotic dynamics.
- Unusual absorption signatures provide new avenues for experimental verification.
Related Concept Videos
Damped Oscillations
In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Although friction and other non-conservative...
Types of Damping
If the amount of damping in a system is gradually increased, the period and frequency start to become affected because damping opposes, and hence slows, the back and forth motion (the net force is smaller in both directions). If there is a very large amount of damping, the system does not even oscillate; instead, it slowly moves toward equilibrium. In brief, an overdamped system moves slowly towards equilibrium, whereas an underdamped system moves quickly to equilibrium but will oscillate about...
Forced Oscillations
When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
Equation of Rotational Dynamics
Angular variables are introduced in rotational dynamics. Comparing the definitions of angular variables with the definitions of linear kinematic variables, it is seen that there is a mapping of the linear variables to the rotational ones. Linear displacement, velocity, and acceleration have their equivalents in rotational motion, which are angular displacement, angular velocity, and angular acceleration. Similar to the rotational variables, a mapping exists from Newton's second law of motion...
Euler Equations of Motion
Imagine a rigid body that is rotating at an angular velocity of ω within an inertial frame of reference. Along with this, picture a second rotating frame that is attached to the body itself. This frame moves along with the body and possesses an angular velocity of Ω. The total moment about the center of mass is calculated by adding the rate of change of angular momentum about the center of mass in relation to the rotating frame and the cross-product of the body's angular velocity and its...
Mechanical Systems
Mechanical systems are analogous to to electrical networks where springs and masses play similar roles to inductors and capacitors, respectively. A viscous damper in mechanical systems functions similarly to a resistor in electrical networks, dissipating energy. The forces acting on a mass in such systems include an applied force in the direction of motion, counteracted by forces from the spring, a viscous damper, and the mass's acceleration. This interplay of forces is mathematically described...

