色散衰减介质中脉冲电磁波束场的角谱表示和谢尔曼展开

K. Oughstun
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引用次数: 6

摘要

脉冲电磁波束场在占据半空间的色散衰减介质中传播的平面波的角谱表示波场为均匀平面波和非均匀平面波的叠加。将无损介质中无源波场的谢尔曼展开推广到有损、色散介质中,从脉冲无源电磁波束场的角谱表示推导出其空间序列表示。这个空间序列表示通过单一轮廓积分明确地显示了脉冲光束场的时间演变,该积分的形式与在有损耗的色散介质中以正z方向传播的脉冲平面波场的傅里叶-拉普拉斯描述中获得的形式相同。通过场边界值的导数,发现脉冲的时间演化依赖于光束场的横向空间位置。
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The angular spectrum representation and the Sherman expansion of pulsed electromagnetic beam fields in dispersive, attenuative media
The angular spectrum of plane-waves representation of a pulsed electromagnetic beam field propagating in a dispersive, attenuative medium occupying the half-space expresses that wave field as a superposition of both homogeneous and inhomogeneous plane waves. A generalization of the Sherman expansion for source-free wave fields in lossless media to the lossy, dispersive medium case is used to derive a spatial series representation of a pulsed, source-free electromagnetic beam field from its angular spectrum representation. This spatial series representation displays the temporal evolution of the pulsed beam field explicitly through a single-contour integral that is of the same form as that obtained in the Fourier-Laplace description of a pulsed plane-wave field that is propagating in the positive z-direction in the lossy, dispersive medium. The temporal pulse evolution is found to depend upon the transverse spatial position in the beam field through the derivatives of the field boundary values.
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