2012
DOI: 10.1109/tmtt.2012.2184129
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Stability and Bifurcation Analysis of Self-Oscillating Quasi-Periodic Regimes

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Cited by 27 publications
(9 citation statements)
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“…The multi-valued solutions are particularly common in oscillator circuits, since the active-device negative conductance often exhibits a nonmonotonous variation with the excitation amplitude [39]. In fact, the device conductance may become more negative in some amplitude intervals, though finally increasing, from a certain amplitude value [39], as expected in physical devices. The multivalued behavior is often observed near the oscillation edges (primary Hopf bifurcations), as shown in Fig.…”
Section: A Hysteresismentioning
confidence: 97%
“…The multi-valued solutions are particularly common in oscillator circuits, since the active-device negative conductance often exhibits a nonmonotonous variation with the excitation amplitude [39]. In fact, the device conductance may become more negative in some amplitude intervals, though finally increasing, from a certain amplitude value [39], as expected in physical devices. The multivalued behavior is often observed near the oscillation edges (primary Hopf bifurcations), as shown in Fig.…”
Section: A Hysteresismentioning
confidence: 97%
“…In Class-D amplifiers, a high amplitude signal (switching signal) at the frequency f o makes the transistors switch between on-and off-stages and the output voltage has a rectangular waveform. In the case of a SOPA, the Class-D amplifier [32][33][34] is inserted into a feedback loop (Fig. 8), which should enable an oscillation at f o , with no need for an extra source.…”
Section: Envelope Transientmentioning
confidence: 99%
“…Fig. 9 presents the output power spectrum obtained with WCDMA-like signal centred at 200 MHz [34]. It shows the dithering effect of the higher frequency oscillation.…”
Section: Envelope Transientmentioning
confidence: 99%
“…When increasing (decreasing) the parameter from a low (high) value the circuit initially operates in section 1 (section 3) and jumps to section 3 (section 1) at the turning point T 1 (T 2 ). In most cases, the hysteresis is due to an expansion of the circuit negative resistance in a certain interval of the excitation amplitude [5], which enables the fulfilment of the steady-state conditions for three distinct amplitude values. In most previous works, hysteresis was undesired, so several simulation tools [1]- [3] were proposed for its accurate prediction at the design stage.…”
Section: Introductionmentioning
confidence: 99%