2014
DOI: 10.1007/s10825-014-0651-3
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Noise in oscillators: a review of state space decomposition approaches

Abstract: We review the state space decomposition techniques for the assessment of the noise properties of autonomous oscillators, a topic of great practical and theoretical importance for many applications in many different fields, from electronics, to optics, to biology. After presenting a rigorous definition of phase, given in terms of the autonomous system isochrons, we provide a generalized projection technique that allows to decompose the oscillator fluctuations in terms of phase and amplitude noise, pointing out … Show more

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Cited by 13 publications
(13 citation statements)
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“…Thus, the gradient vectors of the phase and amplitudes evaluated on χ are left eigenvectors of the monodromy matrix, which are called the adjoint covariant Lyapunov vectors [45][46][47] .…”
Section: Reduction Framework and A Methods To Calculate The Respomentioning
confidence: 99%
“…Thus, the gradient vectors of the phase and amplitudes evaluated on χ are left eigenvectors of the monodromy matrix, which are called the adjoint covariant Lyapunov vectors [45][46][47] .…”
Section: Reduction Framework and A Methods To Calculate The Respomentioning
confidence: 99%
“…We assume that (27) admits of an asymptotically stable Tperiodic solution x s (t), represented by a limit cycle in its state space. We shall derive an equivalent description of system (25) (or (26)) in terms of phase and amplitude deviation variables, analogous to the one derived in [18], [26], [27]. The phase function used in our description coincides locally, in the neighborhood of the limit cycle, with the asymptotic phase defined in [6], [13], [28].…”
Section: Oscillators With Colored Noisementioning
confidence: 99%
“…For our purpose it is more convenient to work with the Itô SDE (26). The reason to prefer the Itô over the Stratonovich interpretation is that Itô integrals are adapted processes, i.e.…”
Section: Oscillators With Colored Noisementioning
confidence: 99%
“…white noise Substituting the defined A and B in (21) and simplifying the terms leads to ln τ 2 + 1 2 > ln τ (22) Knowing that ln e 1/2 = 1/2, the condition of (22) is simplified to τ < τ 2 e. Therefore, it can be concluded that in order to calculate the normalised phase variance of the Flicker noise for the known τ 1 and τ 2 , the parameter τ must satisfy τ 1 < τ < τ 2 e. The PSD of the Flicker noise is S 1/ f ( f ) = S ⋅ f −1 . Comparing this PSD with (11), the normalising factor is X 2 = Sln(τ 2 /τ 1 ).…”
Section: Lorentzian Noise ( F −2 )mentioning
confidence: 99%