Imaging-spectroscopy of a band-split type II solar radio burst with the Murchison Widefield Array

被引:8
|
作者
Bhunia, Shilpi [1 ,2 ]
Carley, Eoin P. P. [1 ]
Oberoi, Divya [3 ]
Gallagher, Peter T. T. [1 ]
机构
[1] Dublin Inst Adv Studies, Astron & Astrophys Sect, Dublin D02 XF86, Ireland
[2] Trinity Coll Dublin, Sch Phys, Coll Green, Dublin, Ireland
[3] Tata Inst Fundamental Res, Natl Ctr Radio Astrophys, Pune 411007, Maharashtra, India
关键词
techniques; imaging spectroscopy; Sun; activity; shock waves; turbulence; SPATIALLY-RESOLVED OBSERVATIONS; CORONAL MAGNETIC-FIELD; SHOCK-WAVES; ELECTRON ACCELERATION; SCATTERING; PROPAGATION; TURBULENCE; EMISSION; CME; CALIBRATION;
D O I
10.1051/0004-6361/202244456
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Type II solar radio bursts are caused by magnetohydrodynamic (MHD) shocks driven by solar eruptive events such as coronal mass ejections (CMEs). Often, both fundamental and harmonic bands of type II bursts are split into sub-bands, which are generally believed to be coming from upstream and downstream regions of the shock; however, this explanation remains unconfirmed. Here, we present combined results from imaging analyses of type II radio burst band splitting and other fine structures observed by the Murchison Widefield Array (MWA) and extreme ultraviolet observations from Solar Dynamics Observatory (SDO)/Atmospheric Imaging Assembly (AIA) on 28 September 2014. The MWA provides imaging-spectroscopy in the range 80-300 MHz with a time resolution of 0.5 s and frequency resolution of 40 kHz. Our analysis shows that the burst was caused by a piston-driven shock with a driver speed of similar to 112 km s(-1) and shock speed of similar to 580 km s(-1). We provide rare evidence that band splitting is caused by emission from multiple parts of the shock (as opposed to the upstream-downstream hypothesis). We also examine the small-scale motion of type II fine structure radio sources in MWA images, and suggest that this motion may arise because of radio propagation effects from coronal turbulence, and is not due to the physical motion of the shock location. We present a novel technique that uses imaging spectroscopy to directly determine the effective length scale of turbulent density perturbations, which is found to be 1-2 Mm. The study of the systematic and small-scale motion of fine structures may therefore provide a measure of turbulence in different regions of the shock and corona.
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页数:10
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