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首页> 外文期刊>International Journal of Electronics >Cherenkov radiation in a plasma-filled coaxial cylindrical dielectric slow-wave structure
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Cherenkov radiation in a plasma-filled coaxial cylindrical dielectric slow-wave structure

机译:等离子体填充同轴圆柱电介质慢波结构中的切伦科夫辐射

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In this paper, a new type of plasma-filled coaxial cylindrical dielectric slow-wave structure that is very beneficial to the beam-wave interaction of the high-power microwave source is developed. The Cherenkov radiation in the plasma-filled coaxial cylindrical dielectric slow-wave structure is examined by use of the self-consistent linear field theory. The dispersion equation and the synchronized condition as well as the wave growth rate of the beam-wave interaction are derived. The dispersion equation clearly shows that the Cherenkov radiation excited in the plasma-filled coaxial cylindrical dielectric slow-wave structure results from the coupling between the slow electromagnetic wave, TM-modes, propagated along the slow-wave structure and the negative-energy space-charge wave propagated along the relativistic electron beam. The numerical results indicate that the dispersion curves are divided into two branches due to the presence of the background plasma in the coaxial cylindrical dielectric slow-wave structure for the identical electromagnetic wave mode, and the radial distributions of the longitudinal fluctuating electric field corresponding to the two dispersion curve branches are completely different. Injection of the background plasma into the slow-wave structure can enhance the output frequency and the wave growth rate of the beam-wave interaction and enables the high-power microwave source that utilizes this kind of slow-wave structure to gain more output power of the microwave with higher output frequency.
机译:本文研究了一种新型的等离子填充同轴圆柱电介质慢波结构,该结构非常有利于大功率微波源的束波相互作用。利用自洽线性场理论研究了等离子体填充的同轴圆柱电介质慢波结构中的切伦科夫辐射。推导了色散方程和同步条件以及束波相互作用的波增长率。色散方程清楚地表明,在等离子体填充的同轴圆柱电介质慢波结构中激发的Cherenkov辐射是由沿着慢波结构传播的慢电磁波TM模式与负能量空间之间的耦合产生的。电荷波沿着相对论电子束传播。数值结果表明,在相同的电磁波模式下,由于同轴圆筒形介质慢波结构中存在背景等离子体,因此色散曲线分为两个分支,并且纵向波动电场的径向分布对应于两个色散曲线分支完全不同。将本底等离子体注入慢波结构可以提高输出频率和束波相互作用的波增长率,并使利用这种慢波结构的高功率微波源获得更多的输出功率。输出频率更高的微波。

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