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本文研究了磁化不均匀等离子体共振点以上的过密区的场分布。由于异常模电磁波与等离子体纵波间的相互转换,电磁波在过密区将再次被激发。The field structures in the overdense region above the resonant paint of an inhomogeneous magnetized plasma are studied. Our work indicates that owing to the mutual conversion be-tween the extraordinary electromagnetic wave and the longitudinal plasma wave, the electromagnetic wave will grow again in the overdense plasma.







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