论文标题
在立体声时代观察到的彩带波事件的特性
Properties of Streamer Wave Events Observed During the STEREO Era
论文作者
论文摘要
通常在冠状质量弹出(CME)之后,有时会在太阳头盔彩带中观察到横向波。 CME驱动的冲击波向侧面移动流板,并在CME通道后观察到流板的衰减振荡。以前的工作通常报道了从单个有利位置(通常是SOHO航天器)采取的流媒体振荡的观察结果。我们进行了数据调查,以搜索由立体声航天器上的Cor2 Coronagraph观察到的流媒体波事件。我们首次通过在立体A和B上使用COR2仪器以及SOHO/LASCO C2+C3 CORONAGRAPHS来报告从多个有利位点观察到流媒体波事件的观察结果。我们通过比较不同的事件并进行统计分析来研究彩带波的特性。常见的观察特征使我们对彩带波事件的物理性质有了更多的了解。最重要的结论是,CME的速度与所得流媒体波的相位速度之间似乎没有关系,这表明流媒体波速度由流媒体的物理性质而不是CME的属性确定。该结果使流媒体波浪事件出色的冠状动脉学研究候选人。根据测量的相位速度与从测量周期和波长计算出的相位速度之间的比较,我们可以确定流媒体中的震后太阳风流的速度约为300 $ \ mathrm {km \ s}}^{ - 1} $。
Transverse waves are sometimes observed in solar helmet streamers, typically after the passage of a coronal mass ejection (CME). The CME-driven shock wave moves the streamer sideways, and a decaying oscillation of the streamer is observed after the CME passage. Previous works generally reported observations of streamer oscillations taken from a single vantage point (typically the SOHO spacecraft). We conduct a data survey searching for streamer wave events observed by the COR2 coronagraphs onboard the STEREO spacecraft. For the first time, we report observations of streamer wave events from multiple vantage points, by using the COR2 instrument on both STEREO A and B, as well as the SOHO/LASCO C2+C3 coronagraphs. We investigate the properties of streamer waves by comparing the different events and performing a statistical analysis. Common observational features give us additional insight on the physical nature of streamer wave events. The most important conclusion is that there appears to be no relation between the speed of the CME and the phase speed of the resulting streamer wave, indicating that the streamer wave speed is determined by the physical properties of the streamer rather than the properties of the CME. This result makes streamer waves events excellent candidates for coronal seismology studies. From a comparison between the measured phase speeds and the phase speeds calculated from the measured periods and wavelengths, we could determine that the speed of the post-shock solar wind flow in our streamers is around 300 $\mathrm{km \ s}^{-1}$.