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Titlebook: Quasi-Optical Control of Intense Microwave Transmission; Proceedings of the N Jay L. Hirshfield,Michael I. Petelin Conference proceedings 2

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樓主: encroach
41#
發(fā)表于 2025-3-28 18:26:01 | 只看該作者
QUASI-OPTICAL TRANSMISSION LINES ATCIEMAT AND AT GPI, simplicity of the launching systems and the big progress in the development of powerful microwave sources and high power transmission systems made this heating method very attractive for many fusion experiments [1, 2].
42#
發(fā)表于 2025-3-28 21:42:59 | 只看該作者
QUASI-OPTICAL MULTIPLEXERS FOR SPACE COMMUNICATION AND RADAR WITH SYNTHESIZED FREQUENCY BAND,d communication should be quite different. In the radar with synthesized frequency band, an adaptive spectrum regularization algorithm provides automatic shrinkage of the range resolution scale with the target approaching.
43#
發(fā)表于 2025-3-28 23:45:50 | 只看該作者
HIGH-POWER MILLIMETREWAVE TRANSMISSION SYSTEMS AND COMPONENTS FOR ELECTRON CYCLOTRON HEATING OF FUS [1] which is currently built at the Max-Planck-Institute for Plasma Physics (IPP) in Greifswald. There, the millimetre wave power of 10 gyrotrons will be transmitted fully optically via two multi-beam waveguides (MBWG)
44#
發(fā)表于 2025-3-29 06:17:54 | 只看該作者
45#
發(fā)表于 2025-3-29 07:20:22 | 只看該作者
OVERSIZED TRANSMISSION LINES FOR GYROTRON-BASED TECHNOLOGICAL OVENS AND PLASMA-CHEMICAL REACTORS,d coatings, rapid annealing of semiconductors, microwave plasma assisted chemical vapor deposition, and multiply charged ion production are among the most advanced developments. The paper presents the status and examples of transmission line developments for such gyrotron-based systems.
46#
發(fā)表于 2025-3-29 15:07:32 | 只看該作者
47#
發(fā)表于 2025-3-29 16:06:53 | 只看該作者
48#
發(fā)表于 2025-3-29 21:05:43 | 只看該作者
49#
發(fā)表于 2025-3-30 01:24:20 | 只看該作者
50#
發(fā)表于 2025-3-30 04:48:48 | 只看該作者
A GENERAL PURPOSE ELECTROMAGNETIC CODE FOR DESIGNING MICROWAVE COMPONENTS,dependent fields. The objects may contain linear dielectric and magnetic materials as well as lossy materials, open boundaries, and may be periodic in three dimensions. Scattering parameters are computed via an FFT of the impulse response. In the time domain, the excitation is by port modes, by rela
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