Abstract
We develop a theoretical framework for analyzing the nonlinear dynamics of a lightly damped Duffing resonator driven by two near-resonant tones, where the two tones are separated into a primary drive and a secondary, significantly weaker drive. In the limit of weak damping and weak secondary drive, the dynamics in a frame rotating with the primary drive frequency are predominantly Hamiltonian, allowing the motion to be analyzed via perturbation techniques. Slow-time equations for the amplitude and phase of the response in the rotating frame are derived using averaging, revealing that the system behaves as an effective “rotating-frame resonator.” The resulting amplitude-phase equations are formally equivalent to those of a single-tone-driven Duffing oscillator, enabling the use of established analytical techniques to characterize the dynamics. The theory predicts steady-state oscillations, resonance conditions, and the nonlinear frequency response of the sidebands generated by the secondary drive. Comparison with experimental measurements from a two-tone-driven nanomechanical beam shows excellent agreement with the predicted amplitude response curves. The presented framework provides a unified, physically intuitive description of the response in the rotating frame relevant to the formation of fine-structure frequency combs, pump-probe optical spectroscopy, resonance-induced damping, and other applications.
| Original language | English |
|---|---|
| Article number | 120020 |
| Journal | Journal of Sound and Vibration |
| Volume | 643 |
| DOIs | |
| State | Published - 24 Nov 2026 |
Keywords
- Lightly perturbed Hamiltonian dynamics
- Nanomechanical resonator
- Nonlinear dynamics in the rotating frame
- Two-tone-driven resonator
ASJC Scopus subject areas
- Condensed Matter Physics
- Acoustics and Ultrasonics
- Mechanics of Materials
- Mechanical Engineering
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