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首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Characteristics of electron cyclotron harmonic waves observed in an active two-point propagation experiment in the ionosphere
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Characteristics of electron cyclotron harmonic waves observed in an active two-point propagation experiment in the ionosphere

机译:电离层主动两点传播实验中观察到的电子回旋加速器谐波特征

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摘要

Electrostatic electron cyclotron waves (ECWs), also-called electron Bernstein waves, observed at harmonics nf c of the electron cyclotron frequency f c were transmitted over field-aligned emitter-receiver separations of hundreds of meters in the active rocket experiment OEDIPUS-C. Although the 300-μs rectangular current pulses into the emitting antenna were smoothly maintained during the experiment, the resulting ECW pulses at the receiver exhibited considerable variety in both the time and frequency domains. A full hot-plasma dispersion relation has been applied to ray-tracing investigations to identify the rays that could connect the emitter and receiver in a smoothly varying model of the auroral ionospheric magnetoplasma. Theoretical connecting rays were limited to frequencies extending from 1 to a few kilohertz above 2f c , which was about 2.6 MHz. But the observed pulse spectra extended over a much broader bandwidth, from several kilohertz below nf c to several kilohertz above, for n = 2, 3, and 4. The broadening is interpreted as a consequence of Doppler effect caused by payload motion and backscatter of the ECWs. Field-aligned density irregularities typical of the auroral topside ionosphere or waves nonlinearly induced by the intense near fields of the HEX antenna may act as the scatterers.
机译:在主动火箭实验OEDIPUS-C中,在电子回旋加速器频率f c的谐波nf c处观察到的静电电子回旋加速器波(ECW)在数百米的场定向发射器-接收器间隔上传输。尽管在实验过程中可以平稳地保持进入发射天线的300μs矩形电流脉冲,但在接收器处产生的ECW脉冲在时域和频域均表现出相当大的变化。完整的热等离子体弥散关系已应用于射线追踪研究,以识别可以在极光电离层磁等离子体的平稳变化模型中连接发射器和接收器的射线。理论连接射线被限制在2f c以上从1到几千赫兹的频率范围内,大约为2.6 MHz。但是对于n = 2、3和4,观察到的脉冲频谱在从nf c以下的几千赫兹到在nf c以下的几千赫兹的更宽的带宽上扩展。这种扩展被解释为由有效载荷运动和反向散射引起的多普勒效应的结果。 ECW。极光顶电离层的典型场对准密度不规则性或由HEX天线的强近场非线性感应产生的波可充当散射体。

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