1991
DOI: 10.1070/qe1991v021n01abeh003726
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Phase effects in passive nonlinear resonators

Abstract: Abshaet We present a long-range hopping tight-binding model in which the ensemble averaged density of states, p(E), undergoes a gradual transition from a homogenous form with almost no variation to swngly peaked behaviour as an external e l d c field grows. The model consists of N x N band random "ices of bandwidth b. The carresponding rnauix elements. h,j. have all vanishing average except on the diagonal where, (hi;) = ari. Here, the parameter o! plays the role of the electric field. We approximate the behav… Show more

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Cited by 4 publications
(4 citation statements)
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“…Such a behaviour is exhibited by the solutions to the oscillation equations in the adiabatically-stratified part of the solar convective envelope, owing to their high-frequency asymptotic properties (the wave propagation here is close to that of purely acoustic waves). Specifically, the near-harmonic behavior is exhibited with best accuracy by eigenfunction ψp(τ ) defined as (see Vorontsov 1991, and Paper I)…”
Section: The Group Velocitymentioning
confidence: 99%
“…Such a behaviour is exhibited by the solutions to the oscillation equations in the adiabatically-stratified part of the solar convective envelope, owing to their high-frequency asymptotic properties (the wave propagation here is close to that of purely acoustic waves). Specifically, the near-harmonic behavior is exhibited with best accuracy by eigenfunction ψp(τ ) defined as (see Vorontsov 1991, and Paper I)…”
Section: The Group Velocitymentioning
confidence: 99%
“…Nevertheless, it is a first approximation. A generalization at second order has been developed for both high (Vorontsov 1991) and low degree modes (Lopes & Turck-Chieze 1994) that find better evidence about the role of the sub surface layers and of the gravity in the core when one can only measure low degree modes; this will be used soon for solar-like stars.…”
Section: The Solar Acoustic Modesmentioning
confidence: 99%
“…In the one-pass resonator model the phase modulation dynamics u = u(t; K) = u(x, y, t; K) is described by the quasilinear diffusion equation [2] ∂ t u + u − D∆u = K(x, y) (1 + γ cos(u + ϕ)) .…”
Section: Introductionmentioning
confidence: 99%