Abstract:Abstract-The dynamics of the onset of oscillations in a wave guide cavity based Gunn Oscillator (GO) has been critically examined through numerical simulations and experimental studies.The transition of the GO from a non-oscillatory to an oscillatory state and the same in the reverse direction occurs at different critical values of the dc bias voltage applied to the GO. In presence of a weak RF field in GO cavity, oscillations with broad band continuous spectrum and multiple discrete line spectrum are observed… Show more
“…Among these parameters, c is most sensitive to bias voltage variation. So the tuning of value of c is taken in simulation study [17]. Values of Ω and q s are taken equal to 1.27 and 0.15 for a set of simulation.…”
Section: Numerical Simulation and Resultsmentioning
confidence: 99%
“…Forcing it by an external signal of amplitude and normalized frequency, q s and Ω, respectively, one gets chaotic oscillations. Thus the equation of GO capable of producing chaotic oscillations is [17],…”
Section: System Equation Of a Chaotic Go (Cgo)mentioning
confidence: 99%
“…As such, nonlinear dynamics of forced GOs has drawn attention of the researchers [14][15][16]. Experimental studies presented in [17] have shown that building up and quenching phenomena of oscillation in a GO due to the variation of operating dc bias voltage show hysteresis. Also an under-biased GO (i.e., a GO biased below the threshold dc bias voltage required for normal oscillation) breaks into chaotic oscillation under the influence of an external periodic signal of appropriate frequency.…”
Abstract-We have studied dynamics of a periodic X-band Gunn oscillator (GO) forced by microwave chaotic signals through numerical simulation and by hardware experiment. The chaos used as forcing signal is generated in a periodically driven non-oscillatory GO. Numerical simulation results indicate that the forced periodic GO becomes chaotic for a moderate strength of forcing chaos. The generated chaos in driven GO is found to become phase or general synchronized to the forcing chaos depending on strength of the latter one. Hardware experiments are performed in X-band of microwave frequency. It shows generation of chaos in driven GO due to forcing. Moreover, synchronization between forcing and generated chaos is indirectly verified.
“…Among these parameters, c is most sensitive to bias voltage variation. So the tuning of value of c is taken in simulation study [17]. Values of Ω and q s are taken equal to 1.27 and 0.15 for a set of simulation.…”
Section: Numerical Simulation and Resultsmentioning
confidence: 99%
“…Forcing it by an external signal of amplitude and normalized frequency, q s and Ω, respectively, one gets chaotic oscillations. Thus the equation of GO capable of producing chaotic oscillations is [17],…”
Section: System Equation Of a Chaotic Go (Cgo)mentioning
confidence: 99%
“…As such, nonlinear dynamics of forced GOs has drawn attention of the researchers [14][15][16]. Experimental studies presented in [17] have shown that building up and quenching phenomena of oscillation in a GO due to the variation of operating dc bias voltage show hysteresis. Also an under-biased GO (i.e., a GO biased below the threshold dc bias voltage required for normal oscillation) breaks into chaotic oscillation under the influence of an external periodic signal of appropriate frequency.…”
Abstract-We have studied dynamics of a periodic X-band Gunn oscillator (GO) forced by microwave chaotic signals through numerical simulation and by hardware experiment. The chaos used as forcing signal is generated in a periodically driven non-oscillatory GO. Numerical simulation results indicate that the forced periodic GO becomes chaotic for a moderate strength of forcing chaos. The generated chaos in driven GO is found to become phase or general synchronized to the forcing chaos depending on strength of the latter one. Hardware experiments are performed in X-band of microwave frequency. It shows generation of chaos in driven GO due to forcing. Moreover, synchronization between forcing and generated chaos is indirectly verified.
“…The coefficients a, b, c, d are related with the device and the cavity parameters and implicitly depend on the magnitude of the applied dc bias (V B ) across the Gunn diode [20].…”
Section: Description Of the Bccgo System And Its Circuit Theoretic Modelmentioning
confidence: 99%
“…As a logical extension of the studies on the BCPGO [14], one may question on the modification of the dynamics of the system if the GOs become chaotic. Adopting the simple method reported in [20] a BCPGO can be converted into a BCCGO system. Here, the GOs would be operated in the under bias condition and a weak external RF field would be injected in the cavities.…”
Abstract-The dynamics of a system of two bilaterally coupled chaotically oscillating X-band Gunn oscillators (GOs) has been studied by numerical simulation and by hardware experiment. The effect of variation of the coupling strengths between two oscillators in two paths has been explored. The chaotic oscillations in two GOs have become synchronized in most of the cases when coupling factors (CFs) are around 20% or more. However, the transformation of chaotic states of the GOs to quasi-periodic ones has been observed for some values of CFs. A detailed numerical analysis on the instantaneous error parameters of the GO state variables is presented to identify different steady state dynamical conditions of the system. Experimental observations of the GO output frequency power spectra and the averaged product of the two GO outputs in the coupled mode confirm the occurrence of synchronization as well as quenching of chaotic oscillations for different values of CFs.
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