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首页> 外文期刊>The Astrophysical journal >ION ACOUSTIC WAVE FREQUENCIES AND ONSET TIMES DURING TYPE Ⅲ SOLAR RADIO BURSTS
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ION ACOUSTIC WAVE FREQUENCIES AND ONSET TIMES DURING TYPE Ⅲ SOLAR RADIO BURSTS

机译:Ⅲ型太阳无线电爆发期间的离子声波频率和起振时间

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Conflicting interpretations exist for the low-frequency ion acoustic (S) waves often observed by ISEE 3 in association with intense Langmuir (L) waves in the source regions of type Ⅲ solar radio bursts near 1 AU. Two indirect lines of observational evidence, as well as plasma theory, suggest they are produced by the electrostatic (ES) decay L → L′ + S. However, contrary to theoretical predictions, an existing analysis of the wave frequencies instead favors the electromagnetic (EM) decays L → T + S, where T denotes an EM wave near the plasma frequency. This conflict is addressed here by comparing the observed wave frequencies and onset times with theoretical predictions for the ES and EM decays, calculated using the time-variable electron beam and magnetic field orientation data, rather than the nominal values used previously. Field orientation effects and beam speed variations are shown analytically to produce factor-of-three effects, greater than the difference in wave frequencies predicted for the ES and EM decays; effects of similar magnitude occur in the events analyzed here. The S-wave signals are extracted by hand from a sawtooth noise background, greatly improving the association between S waves and intense L waves. Very good agreement exists between the time-varying predictions for the ES decay and the frequencies of most (but not all) wave bursts. The waves occur only after the ES decay becomes kinematically allowed, which is consistent with the ES decay proceeding and producing most of the observed signals. Good agreement exists between the EM decay's predictions and a significant fraction of the S-wave observations while the EM decay is kinematically allowed. The wave data are not consistent, however, with the EM decay being the dominant nonlinear process. Often the observed waves are sufficiently broadband to overlap simultaneously the frequency ranges predicted for the ES and EM decays. Coupling the dominance of the ES decay with this frequency overlap provides support for a previous suggestion that fundamental emission occurs when the EM decay is stimulated by the ES decay product waves. The periods in which the ES and EM decays produce observable S waves are consistent with the observed and (independently) predicted times of fundamental and harmonic radio emission. This supports interpretation of fundamental emission as stimulated EM decay and harmonic emission as the coalescence L + L′ → T of beam-generated L waves and L′ waves produced by the ES decay, where T denotes an electromagnetic wave at twice the plasma frequency. Analysis of the electron beam data reveals that the time-varying beam speed is consistent with ballistic beam propagation with minimal energy loss, implying that the beam propagates in a state close to time- and volume-averaged marginal stability. This confirms a central tenet of the stochastic growth theory for type Ⅲ bursts. The observational data are thus shown to be uniformly consistent with the ES decay being the dominant nonlinear process for type Ⅲ bursts near 1 AU, as expected theoretically. Further work is required to determine whether the ES decay appreciably limits the beam's energy loss over and above the effects of linear stochastic growth theory.
机译:对于经常被ISEE 3观察到的低频离子声(S)波与在1 AU附近的Ⅲ型太阳射电爆发源区域中的强烈朗缪尔(L)波相关的解释存在矛盾。两条间接的观测证据线以及等离子理论表明,它们是由静电(ES)衰减L→L'+ S产生的。但是,与理论预测相反,对波频率的现有分析反而倾向于电磁波(ES)。 EM)衰减L→T + S,其中T表示接近等离子频率的EM波。通过将观察到的波频率和开始时间与ES和EM衰减的理论预测值进行比较,可以解决此冲突,该预测是使用时变电子束和磁场方向数据而不是先前使用的标称值来计算的。分析性地显示了场定向效应和射束速度变化以产生三因子效应,该效应大于为ES和EM衰减预测的波频率差;在这里分析的事件中,发生了相似大小的影响。手动从锯齿形噪声背景中提取S波信号,从而极大地改善了S波与强L波之间的关联。 ES衰减的时变预测与大多数(但不是全部)波突发的频率之间存在很好的一致性。仅在运动学允许ES衰减之后才出现波,这与ES衰减进行并产生大多数观察到的信号一致。 EM衰减在运动学上是允许的,但在EM衰减的预测与大部分S波观测之间存在良好的一致性。然而,波浪数据并不一致,其中电磁衰减是主要的非线性过程。通常,观察到的波具有足够的宽带,可以同时重叠为ES和EM衰减预测的频率范围。将ES衰减的优势与该频率重叠耦合起来,为先前的建议提供了支持,即当ES衰减积波激发EM衰减时,会发生基本发射。 ES和EM衰减产生可观察到的S波的周期与基波和谐波无线电发射的观测时间和(独立地)预测时间一致。这支持将基本发射解释为受激EM衰减,并将谐波发射解释为束产生的L波和ES衰减所产生的L'波的合并L + L'→T,其中T表示等离子频率两倍的电磁波。对电子束数据的分析表明,时变束速度与弹道束传播一致,且能量损失最小,这意味着束以接近时间和体积平均边际稳定性的状态传播。这证实了Ⅲ型脉冲随机增长理论的中心宗旨。因此,观测到的数据与ES衰减一致,这是理论上所期望的,对于1 AU附近的Ⅲ型爆发,ES衰减是主要的非线性过程。除了线性随机增长理论的影响外,还需要进一步的工作来确定ES衰减是否明显限制了光束的能量损耗。

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