Phase-plane dynamics of an atomic force microscope cantilever.

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SUMMARY

The discussion centers on the phase-plane dynamics of an atomic force microscope (AFM) cantilever, specifically how its motion transitions from ideal sinusoidal oscillations to complex behaviors due to inter-atomic forces. The undisturbed cantilever exhibits elliptical trajectories in the phase-plane, while disturbances can lead to nonlinear phenomena such as period-doubling, bifurcation, and chaos. The user seeks insights into the attractor and basin of attraction related to their experimental data, noting that the phase-plane trajectories evolve from circular patterns to a configuration with two centers as signal size increases.

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  • Understanding of atomic force microscopy (AFM) principles
  • Familiarity with phase-plane analysis
  • Knowledge of nonlinear dynamics and chaos theory
  • Experience with time series analysis techniques
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  • Research "nonlinear dynamics in AFM cantilevers" for advanced insights
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Researchers, physicists, and engineers working with atomic force microscopy, particularly those interested in the dynamics of cantilevers and the implications of nonlinear behaviors in experimental setups.

danber
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Hello,

A sinusoidally driven and undisturbed cantilever of an atomic force microscope (AFM) oscillates ideally in a sinusoidal fashion but the motion of the cantilever (time-domain trajectory) can become more complicated when it is disturbed by the inter-atomic forces as the cantilever taps on the sample surface. The cantilever dynamics can be better understood in the phase-plane. An undisturbed cantilever shows elliptical trajectories in the phase-plane around a center. On the other hand, a disturbed cantilever can show nonlinear effects like period-doubling, bifurcation and chaos.

I'd like to know what can be said about the phase-plane trajectory in terms of the attractor, basin of attraction or the possibility of chaos as shown in the attachement containing my experimental data? In the beginning the phase-plane trajectories circle around a center and as the signal size increases, these trajectories also grow in size and the center transforms into a set of two centers.

Thanks.
 
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Thanks.

I already know the papers by Raman and Jamitzky but they've done experiments aimed at observing chaos in AFM and I've a different experiment where I'm not forcing the cantilever motion to be chaotic but observing breakdown of the cantilever trajectory in time-domain and the phase-plane trajectory shows a specific attractor which doesn't seem to be a chaotic one but still is markedly different from that of a harmonic oscillator.

I think time series analysis of the given experimental data can be helpful but my question was how to understand the attractor from a purly dynamical point of view?
 

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