Direct Estimates of the Solar Coronal Magnetic Field Using Contemporaneous Extreme-ultraviolet, Radio, and White-light Observations

被引:37
作者
Kumari, Anshu [1 ]
Ramesh, R. [1 ]
Kathiravan, C. [1 ]
Wang, T. J. [2 ,3 ]
Gopalswamy, N. [3 ]
机构
[1] Indian Inst Astrophys, 100 Feet Rd,Koramangala 2 Block, Bangalore 560034, Karnataka, India
[2] Catholic Univ Amer, Dept Phys, Washington, DC 20064 USA
[3] NASA, Goddard Space Flight Ctr, Code 671, Greenbelt, MD 20771 USA
关键词
Sun: activity; Sun: corona; Sun: coronal mass ejections (CMEs); Sun: magnetic fields; Sun: radio radiation; SHOCK-WAVES; II BURSTS; EMISSION; SPECTROGRAPH; POLARIZATION; ASSOCIATION;
D O I
10.3847/1538-4357/ab2adf
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We report a solar coronal split-band type II radio burst that was observed on 2016 March 16 with the Gauribidanur Radio Spectro-Polarimeter in the frequency range approximate to 90-50 MHz, and the Gauribidanur RadioheliograPH at two discrete frequencies, viz. 80 and 53.3 MHz. Observations around the same epoch in extreme ultraviolet (EUV) and white light show that the above burst was associated with a flux-rope structure and a coronal mass ejection (CME), respectively. The combined height-time plot generated using EUV, radio, and white-light data suggests that the different observed features (i.e., the flux rope, type II burst, and the CME) are all closely associated. We constructed an empirical model for the coronal electron density distribution (N-e(r), where r is the heliocentric distance) from the above set of observations themselves and used it to estimate the coronal magnetic field strength (B) over the range of r values in which the respective events were observed. The B values are consistent with each other. They vary as B(r) = 2.61 x r(-2.21) G in the range r approximate to 1.1-2.2R(circle dot). As far as we know, similar direct estimates of B in the near-Sun corona without assuming a model for N-e(r), and by combining cotemporal set of observations in two different regions (radio and white-light) of the electromagnetic spectrum, have rarely been reported. Further, the present work is a novel attempt where the characteristics of a propagating EUV flux-rope structure, considered to be the signature of a CME close to the Sun, have been used to estimate B(r) in the corresponding distance range.
引用
收藏
页数:8
相关论文
共 82 条
[1]  
[Anonymous], APJ
[2]  
Aurass H., 1997, Coronal Physics from Radio and Space Observations. Proceedings of the CESRA Workshop, P135
[3]   The coronal mass ejection of 1998 April 20: Direct imaging at radio wavelengths [J].
Bastian, TS ;
Pick, M ;
Kerdraon, A ;
Maia, D ;
Vourlidas, A .
ASTROPHYSICAL JOURNAL, 2001, 558 (01) :L65-L69
[4]  
Baumbach S., 1937, Astron. Nachr., V263, P121
[5]   A World-Wide Net of Solar Radio Spectrometers: e-CALLISTO [J].
Benz, A. O. ;
Monstein, C. ;
Meyer, H. ;
Manoharan, P. K. ;
Ramesh, R. ;
Altyntsev, A. ;
Lara, A. ;
Paez, J. ;
Cho, K.-S. .
EARTH MOON AND PLANETS, 2009, 104 (1-4) :277-285
[6]   The large angle spectroscopic coronagraph (LASCO) [J].
Brueckner, GE ;
Howard, RA ;
Koomen, MJ ;
Korendyke, CM ;
Michels, DJ ;
Moses, JD ;
Socker, DG ;
Dere, KP ;
Lamy, PL ;
Llebaria, A ;
Bout, MV ;
Schwenn, R ;
Simnett, GM ;
Bedford, DK ;
Eyles, CJ .
SOLAR PHYSICS, 1995, 162 (1-2) :357-402
[7]   Magnetic field strength in the solar corona from type II band splitting [J].
Cho, K.-S. ;
Lee, J. ;
Gary, D. E. ;
Moon, Y.-J. ;
Park, Y. D. .
ASTROPHYSICAL JOURNAL, 2007, 665 (01) :799-804
[8]   A HIGH-FREQUENCY TYPE II SOLAR RADIO BURST ASSOCIATED WITH THE 2011 FEBRUARY 13 CORONAL MASS EJECTION [J].
Cho, K. -S. ;
Gopalswamy, N. ;
Kwon, R. -Y. ;
Kim, R. -S. ;
Yashiro, S. .
ASTROPHYSICAL JOURNAL, 2013, 765 (02)
[9]   Low coronal observations of metric type II associated CMEs by MLSO coronameters [J].
Cho, K. -S. ;
Bong, S. -C. ;
Kim, Y. -H. ;
Moon, Y. -J. ;
Dryer, M. ;
Shanmugaraju, A. ;
Lee, J. ;
Park, Y. D. .
ASTRONOMY & ASTROPHYSICS, 2008, 491 (03) :873-882
[10]   On the association between type II radio bursts and CMEs [J].
Classen, HT ;
Aurass, H .
ASTRONOMY & ASTROPHYSICS, 2002, 384 (03) :1098-1106