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Well-defined EUV wave associated with a CME-driven shock

机译:与CME驱动的电击相关的清晰EUV波

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Aims. We report on a well-defined EUV wave observed by the Extreme Ultraviolet Imager (EUVI) on board the Solar Terrestrial Relations Observatory (STEREO) and the Atmospheric Imaging Assembly (AIA) on board the Solar Dynamics Observatory (SDO). The event was accompanied by a shock wave driven by a halo CME observed by the Large Angle and Spectrometric Coronagraph (LASCO-C2/C3) on board the Solar and Heliospheric Observatory (SOHO), as evidenced by the occurrence of type II bursts in the metric and dekameter-hectometric wavelength ranges. We investigated the kinematics of the EUV wave front and the radio source with the purpose of verifying the association between the EUV wave and the shock wave. Methods. The EUV wave fronts were determined from the SDO/AIA images by means of two appropriate directions (slices). The heights (radial propagation) of the EUV wave observed by STEREO/EUVI and of the radio source associated with the shock wave were compared considering the whole bandwidth of the harmonic lane of the radio emission, whereas the speed of the shock was estimated using the lowest frequencies of the harmonic lane associated with the undisturbed corona, using an appropriate multiple of the Newkirk (1961, ApJ, 133, 983) density model and taking into account the H/F frequency ratio f _(H)∕ f _(F)= 2. The speed of the radio source associated with the interplanetary shock was determined using the Mann et al. (1999, A&A, 348, 614) density model. Results. The EUV wave fronts determined from the SDO/AIA images revealed the coexistence of two types of EUV waves, a fast one with a speed of ~560 km s~(?1), and a slower one with a speed of ~250 km s~(?1), which corresponds approximately to one-third of the average speed of the radio source (~680 km s~(?1)). The radio signature of the interplanetary shock revealed an almost constant speed of ~930 km s~(?1), consistent with the linear speed of the halo CME (950 km s~(?1)) and with the values found for the accelerating coronal shock (~535–823 km s~(?1)), taking into account the gap between the radio emissions.
机译:目的我们报告了由太阳地面关系天文台(STEREO)上的极紫外成像仪(EUVI)和太阳动力学天文台(SDO)上的大气成像组件(AIA)观测到的清晰EUV波。该事件伴随着由光晕CME驱动的冲击波,该光波由太阳和日球天文台(SOHO)上的大角度和光谱日冕仪(LASCO-C2 / C3)观测到,这在太阳和天文台上发生了II型爆发。公制和十卡-公制波长范围。我们研究了EUV波前和无线电源的运动学,目的是验证EUV波与冲击波之间的关联。方法。通过两个合适的方向(切片)从SDO / AIA图像确定EUV波前。考虑到无线电发射谐波通道的整个带宽,比较了STEREO / EUVI观测到的EUV波的高度(径向传播)和与冲击波有关的无线电源的高度,而使用使用Newkirk(1961,ApJ,133,983)密度模型的适当倍数并考虑H / F频率比f _(H)∕ f _(F )= 2.使用Mann等人的方法确定与行星际冲击有关的无线电源的速度。 (1999,A&A,348,614)密度模型。结果。根据SDO / AIA图像确定的EUV波阵面揭示了两种类型的EUV波并存,一种快的波速为〜560 km s〜(?1),另一种慢的波速为〜250 km s 〜(?1),大约相当于无线电源平均速度的三分之一(〜680 km s〜(?1))。行星际激波的无线电信号显示出约930 km s〜(?1)的恒定速度,与光晕CME的线速度(950 km s〜(?1))一致,并且与加速时的值一致。考虑到无线电发射之间的差距,进行日冕冲击(〜535–823 km s〜(?1))。

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