The measurement of excitation functions for the strongly dissipative collision with the reaction system of ^19F+^27Al has been carried out at the China Institute of Atoraic Energy, Beijing. The ^19F^8+ beam was extrac...The measurement of excitation functions for the strongly dissipative collision with the reaction system of ^19F+^27Al has been carried out at the China Institute of Atoraic Energy, Beijing. The ^19F^8+ beam was extracted from the HI-13 tandem accelerator. The beam incident energies were varied from 110 to 118.75 MeV in steps of 250 keV. The self-supporting ^27A1 target foil with the thickness of 60μg/cm^2 was used. The detector arrangement is shown in Fig.1.展开更多
It is very easy to design an observer for a discrete chaotic system which possesses one non linear scalar quantity, and one can realize the synchronization between the investigated chaotic system and its observer eas...It is very easy to design an observer for a discrete chaotic system which possesses one non linear scalar quantity, and one can realize the synchronization between the investigated chaotic system and its observer easily. This method is applied to two chaotic systems.展开更多
文摘The measurement of excitation functions for the strongly dissipative collision with the reaction system of ^19F+^27Al has been carried out at the China Institute of Atoraic Energy, Beijing. The ^19F^8+ beam was extracted from the HI-13 tandem accelerator. The beam incident energies were varied from 110 to 118.75 MeV in steps of 250 keV. The self-supporting ^27A1 target foil with the thickness of 60μg/cm^2 was used. The detector arrangement is shown in Fig.1.
文摘It is very easy to design an observer for a discrete chaotic system which possesses one non linear scalar quantity, and one can realize the synchronization between the investigated chaotic system and its observer easily. This method is applied to two chaotic systems.