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In the following, we will investigate the oscillation mode in detail, assuming that we are trying to explain the PP oscillation in terms of the two-room model.
For bounded strongly pseudoconvex domains D with smooth boundary in Cn, we introduce a kind of "mean oscillation" in terms of the Kobayashi metric.
For bounded symmetric domains Ω in Cn, a notion of "bounded mean oscillation" in terms of the Bergman metric is introduced.
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Reference [43] studied the differences between the free and forced oscillations in terms of their energy conversions.
We analyze the spatial patterns of Turing and mixed-mode oscillations in terms of the spatial spectral density of the E-fluctuations.
The present communication discusses the peak shape distortions ("inverted" peaks, current oscillations) in terms of tangential movements of the mercury electrode surface.
Another possible explanation for the occurrence of discrete ULF oscillations in terms of standing magnetospheric surface waves (or Krusukal-Schwarzschild-modes) has recently been suggested (Plaschke et al., 2009a).
In particular, we analytically derive the existence conditions and the profiles of oscillations in terms of reaction kinetic parameters and reveal dimensionless quantities that essentially characterize the oscillatory dynamics.
The nature of oscillations in terms of their amplitude and frequency and their evolution for Type-I and Type-II instabilities are studied with respect to the effect of heater power and pressure.
Epsilon is distinct from other high frequency oscillations in terms of generation mechanisms and location.
Briefly, it consists of evaluating the response of the respiratory system to small amplitude pressure oscillations in terms of impedance (Zrs).
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