Intense microwave generators intended for mass production are characterized by a number of parame� ters, the mass, size, and cost always being the most important among them. The lighter and more inex� pensive a microwave generator, the more attractive it seems to be for potential employment. When we deal with very intense (>1 MW) and superintense (>1 GW) microwave generators, we usually relate them to either electronic devices, such as travelingwave tubes (TWTs), backwardwave tubes (BWTs), klystrons, magnetrons, gyrotrons, virtual cathode oscillators, etc., or plasma devices, e.g., plasmabeam generators. In all of them, the energy of highcurrent electron beams is transformed to micro� waveradiation energy. The necessity to apply electron beams imposes sig� nificant constraints on the exterior characteristics of these generators, in particular, on their mass, size, and cost. For example, in addition to basic systems such as electrodynamic structures and antennas, these gener� ators need rather cumbersome auxiliary equipment. Here, we imply a vacuum system producing a deep vacuum (down to ~10 -5 Torr), a highly efficient cath� ode providing highdensity electronemission current (>10 kA cm -2 ), an intense highvoltage powersupply unit (>100 kV) required to accelerate the electron beam, and an electron collector. A magnetic system providing the presence of the magnetic field (>1 kG) within the entire volume of the electrodynamic system is also required. It is necessary to prevent the electron� beam divergence caused by the Coulomb repulsion. As a result, all these auxiliary systems determine ulti� mately the noticeable mass, size, and cost of the microwave generators. In addition to the information given above, the electrodynamic structures, in themselves, of intense electronic microwave generators, as a rule, are charac� terized by a large size. It is convenient to express the volume V of generator electrodynamic structures in terms of the cubic wavelength λ 3 = (c/F) 3 . Here, c is the speed of light in a vacuum and F is the carrying fre� quency of the microwave radiation generated in the structure. Usually, the volume of an intense electronic microwave generator is V > λ 3 , whereas the volume of a superintense multiwave generator is, often, V > (10λ) 3 . For comparison, we may say that in lowinten� sity semiconductor microwave generators (avalanche� flight diodes, Gunn diodes), the volume of the work� ing generation zone is V λ 3 . Thus, we may call these generators miniature devices.
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