A computer simu1ation of a dc superconducting quantum interference device (dc SQUID) in the case P, 3, Pt. 6.28, and noise parameter I= 0. 01 is performed. The main difference with respect to the case of noiseless behavior is the disappearing and/or mixing of some solutions of the differential equations describing the time evolution of the system. Only by including the noise ef-fect in the simulation is it possible to understand the working mechanism of some practical devices characterized byhigh values of the critical current ...
Noise effect on instabilities and chaotic solutions of a superconducting interferometer
R Leoni;V Foglietti
1987
Abstract
A computer simu1ation of a dc superconducting quantum interference device (dc SQUID) in the case P, 3, Pt. 6.28, and noise parameter I= 0. 01 is performed. The main difference with respect to the case of noiseless behavior is the disappearing and/or mixing of some solutions of the differential equations describing the time evolution of the system. Only by including the noise ef-fect in the simulation is it possible to understand the working mechanism of some practical devices characterized byhigh values of the critical current ...File in questo prodotto:
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