By M. Mukerjee
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Extra resources for Adv. Microwave and Millimeter Wave Techs - Devices, Circs and Systems
E. energies per irradiated surface unit) in the order of 5 to 9 J/cm². The plasma plume expands in the ambient oxygen atmosphere (total Exploiting the semiconductor-metal phase transition of VO2 materials: a novel direction towards tuneable devices and systems for RFmicrowave applications 39 pressure in the chamber maintained at 2×10-2 mbar). , 2004). The substrate is heated by an halogen lamp at about 500°C and the deposition duration is changing from 10 to 45 minutes leading to thickness in the range 100 - 600 nm.
19. X-ray of initial stage of a jet formation from W-type liner. Fig. 20. Simulation of the FCG operation developed under the scientific leadership of Prof. Minin. Other aspect of the future explosive plasma antenna development is as follows. Pulse power levels obtained now have the units of GW values. That power is determined by high values of the antenna input voltage (units of megavolts). It can leads to breakdowns in the feeder and antenna. Such a problem also arise in the making of mobile sources that have power of tens megawatt value.
Minin  at the beginning of 1960th discovered a new shaped charge with cylindrical liner [13, 29]. Such type of shaped charge could be also applied to plasma antenna design (figure 17). Explosive pulsed plasma antennas for information protection 29 Fig. 16. Dielectric shaped charge antenna. Fig. 17. Plasma dielectric antenna based on shaped charge with cylindrical liner. As it was mentioned below the jet properties depend on the charge case and liner shape, released energy, and the liner mass and composition.
Adv. Microwave and Millimeter Wave Techs - Devices, Circs and Systems by M. Mukerjee