Skip to content
DraconiticResearch
Search Sources API
203,234 studies31 sourcesUpdated 16 min ago
PreprintCC BY 4.0arXiv

Infinite Set of Resonances in the Linear Damped Oscillator Subject to Harmonic Forcing with Non-standard Frequency Modulation

Abstract

It is shown that harmonic signals incorporating a type of weak non-standard frequency modulation (wNSFM) have interesting spectral properties, namely, time-dependent bandwidths that become increasingly broader with increasing time. As such, they represent a class of signals with frequency-time coupling in their spectra. Specifically, the weakly damped oscillator exhibits always two transient resonance captures involving two distinct harmonics possessing relatively high amplitudes over finite time intervals, while the overall response decays as t−1/2 as t→∞. Considering the undamped oscillator, it possesses two types of resonances, referred to as simple and non-simple resonances. Simple resonances correspond to finite-amplitude steady-state responses caused by two sustained resonance captures, in the form of two distinct modulated quasi-periodic responses, which, however are "activated" at different time instances. The necessary and sufficient conditions for non-simple resonances are given in the form of a theorem which predicts the existence of resonant harmonics and specifies the special phase conditions that the resonant harmonics must satisfy for constructive interference; the resulting undamped non-simple resonance grows unboundedly as t−1/2 as t→∞, in contrast to the classical resonance growth of the linear resonator with unmodulated harmonic excitation whose response grows as t as t→∞. These resonant responses are persistent to changes in the parameters of the wNSFM. Our results reveal interesting infinite sets of resonances in linear SDOF resonators under frequency-modulated excitations.

Related

  1. An unified approach for the (inverted) quantum harmonic oscillator and the Berry-Keating hamiltonian
    Fabio Bagarello, Emanuele Balistreri, Sergey Kuzhel
    arXivPreprintarXiv licenceFull textMathematical physicsQuantum physics & quantum informationarXiv
  2. Combinatorics of noncommutative harmonic oscillator determinant
    Masato Wakayama, Wadim Zudilin
    arXivPreprintarXiv licenceFull textAlgebra & number theoryAnalysis & PDEsarXiv
  3. 5D Runge-Lenz Vector from Symplectic Reduction of 8D Harmonic Oscillator
    Hitoshi Ikemori, Shinsaku Kitakado, Yoshimitsu Matsui +2
    arXivPreprintCC BY-NC-ND 4.0Full textMathematical physicsHigh-energy & particle physicsarXiv
  4. On the parabolic Φ34 model for the harmonic oscillator II: global existence and invariant measures
    Aurélien Deya, Reika Fukuizumi, Laurent Thomann
    HALPreprintCC BY 4.0Full textAnalysis & PDEsProbabilityHAL
  5. On the parabolic Φ34 model for the harmonic oscillator II: global existence and invariant measures
    Aurélien Deya, Reika Fukuizumi, Laurent Thomann
    arXivPreprintarXiv licenceFull textAnalysis & PDEsProbabilityarXiv
BibTeX
@misc{gendelman2026infinite,
  title = {{Infinite Set of Resonances in the Linear Damped Oscillator Subject to Harmonic Forcing with Non-standard Frequency Modulation}},
  author = {Oleg V. Gendelman and Luis M. Baldelomar Pinto and Lawrence A. Bergman and Alexander F. Vakakis},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2607.05547},
  eprint = {2607.05547},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2607.05547},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Infinite Set of Resonances in the Linear Damped Oscillator Subject to Harmonic Forcing with Non-standard Frequency Modulation
AU  - Oleg V. Gendelman
AU  - Luis M. Baldelomar Pinto
AU  - Lawrence A. Bergman
AU  - Alexander F. Vakakis
PY  - 2026
DA  - 2026/09/22
PB  - arXiv
DO  - 10.48550/arxiv.2607.05547
UR  - https://arxiv.org/abs/2607.05547
AB  - It is shown that harmonic signals incorporating a type of weak non-standard frequency modulation (wNSFM) have interesting spectral properties, namely, time-dependent bandwidths that become increasingly broader with increasing time. As such, they represent a class of signals with frequency-time coupling in their spectra. Specifically, the weakly damped oscillator exhibits always two transient resonance captures involving two distinct harmonics possessing relatively high amplitudes over finite time intervals, while the overall response decays as t^−1/2 as t→∞. Considering the undamped oscillator, it possesses two types of resonances, referred to as simple and non-simple resonances. Simple resonances correspond to finite-amplitude steady-state responses caused by two sustained resonance captures, in the form of two distinct modulated quasi-periodic responses, which, however are "activated" at different time instances. The necessary and sufficient conditions for non-simple resonances are given in the form of a theorem which predicts the existence of resonant harmonics and specifies the special phase conditions that the resonant harmonics must satisfy for constructive interference; the resulting undamped non-simple resonance grows unboundedly as t^−1/2 as t→∞, in contrast to the classical resonance growth of the linear resonator with unmodulated harmonic excitation whose response grows as t as t→∞. These resonant responses are persistent to changes in the parameters of the wNSFM. Our results reveal interesting infinite sets of resonances in linear SDOF resonators under frequency-modulated excitations.
ER  -