Loading…
Magnetoacoustic Wave Trains in the 11 July 2005 Radio Event with Fiber Bursts
A dm-radio emission with fiber bursts observed on 11 July 2005 was analyzed using wavelet filtration and spectral methods. In filtered radio spectra we found structures with different characteristic period P and frequency drift FD: i ) fiber substructures (composed of dot emissions) with P 1 ≈ 0.5 ...
Saved in:
Published in: | Solar physics 2011-11, Vol.273 (2), p.393-402 |
---|---|
Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
Summary: | A dm-radio emission with fiber bursts observed on 11 July 2005 was analyzed using wavelet filtration and spectral methods. In filtered radio spectra we found structures with different characteristic period
P
and frequency drift FD:
i
) fiber substructures (composed of dot emissions) with
P
1
≈ 0.5 s, FD
1
=− 87 MHz s
−1
on average,
ii
) fiber structures with
P
2
≈1.9 s, and
iii
) drifting structures with
P
3
≈81.4 s, FD
2
=− 8.7, + 98.5, and − 21.8 MHz s
−1
. In the wavelet spectra we recognized patterns having the form of tadpoles. They were detected with the same characteristic periods
P
as found for the filtered structures. The frequency drift of the tadpole heads is found to be equal to the frequency drift of some groups of fibers for the long-period wavelet tadpoles (
P
3
) and to the frequency drift of individual fibers for the short-period tadpoles (
P
2
). Considering these wavelet tadpoles as signatures of propagating magnetoacoustic wave trains, the results indicate the presence of several wave trains in the fibers’ source. While the long-period wave trains trigger or modulate a whole group of fibers, the short-period ones look like being connected with individual fiber bursts. This result supports the model of fibers based on magnetoacoustic waves. Using a density model of the solar atmosphere we derived the velocities of the magnetoacoustic waves, 107 and 562 km s
−1
, and setting them equal to the Alfvén ones we estimated the magnetic field in the source of fiber bursts as 10.7 and 47.8 G. |
---|---|
ISSN: | 0038-0938 1573-093X |
DOI: | 10.1007/s11207-011-9794-6 |