2017
DOI: 10.1109/tmtt.2016.2640955
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Experimental Investigation of Bifurcation Behavior in Nonlinear Microwave Circuits

Abstract: We present an experimental technique to study bifurcations in periodically-forced nonlinear microwave circuits, including even physically unstable (periodic) steady-states. The designer specifies a key node in the circuit being studied (often associated with an active device) and the method synthesizes a voltage waveform to match the waveform at the selected node so that no current flows across the interface. This null condition is maintained while a parameter, such as bias voltage, is varied over a specified … Show more

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Cited by 10 publications
(14 citation statements)
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“…The states S 1 and S 2 are stable, whereas U is unstable. Extending the techniques of [8] to the autonomous case, it is possible to stabilize the oscillator in state U. When the stabilization mechanism is turned off, the oscillator will jump (randomly) to one of the stable states S 1 or S 2 .…”
Section: Coupling-induced Hysteresis In Colpitts Oscillatormentioning
confidence: 99%
“…The states S 1 and S 2 are stable, whereas U is unstable. Extending the techniques of [8] to the autonomous case, it is possible to stabilize the oscillator in state U. When the stabilization mechanism is turned off, the oscillator will jump (randomly) to one of the stable states S 1 or S 2 .…”
Section: Coupling-induced Hysteresis In Colpitts Oscillatormentioning
confidence: 99%
“…can go up or down during the trace, but arc-length increases along the zero curve by construction. As described in the previous work [15], an application of an injection signal with nulled current does not change the state of the DUT, but can change its stability properties. In the case of an autonomous DUT, the frequency and phase of the oscillation of the DUT are determined by the reference oscillator (VCO) because the DUT injection-locks to it.…”
Section: B Numerical Methodsmentioning
confidence: 88%
“…Y  can also be zero at two additional frequencies, below and above n  , as easily gathered from (15). Replacing the three frequencies in ( , ) r T Y V  one obtains three different amplitude values, one for each frequency, which explains the hysteresis induced by linear coupling effects.…”
Section: Multiple Hysteresis Cyclesmentioning
confidence: 99%
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