Do solar decimetric spikes originate in coronal X-ray sources?

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(New page: == Introduction == In the standard solar flare scenario, a large number of particles (electrons and protons) are accelerated in the solar corona. Radiative signatures of those particles a...)
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== Introduction ==
== Introduction ==
In the standard solar flare scenario, a large number of particles (electrons and protons) are accelerated in the solar corona. Radiative signatures of those particles are found in X-rays and radio wavelenghts, teling us the the particles are non-thermally distributed in energy. Assuming that the same distribution of particles causes both, X-ray and radio emission, one would expect a close relation of the two emission types. Indeed, millisecond spikes have been found to have a high temporal association rate with hard X-rays.  
In the standard solar flare scenario, a large number of particles (electrons and protons) are accelerated in the solar corona. Radiative signatures of those particles are found in X-rays and radio wavelenghts, teling us the the particles are non-thermally distributed in energy. Assuming that the same distribution of particles causes both, X-ray and radio emission, one would expect a close relation of the two emission types. Indeed, millisecond spikes have been found to have a high temporal association rate with hard X-rays.  
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By combining RHESSI observations (positions of X-ray sources) with Phoenix-2 data (identification of radio spikes) and observations from the Nancay Radio Heliograph (locations of the radio emission in 4 discrete frequencies) in a particularly well observed limb event we can find - at least one - answer to the above question. Figure one shows the radio spectrogram and the thermal and nonthermal X-ray light curves of the event. The spikes occured in the impulsive phase, when the soft X-ray emission was still rising. However, the radio emission is not clearly correlated with the details of the hard X-ray lightcurve.  
By combining RHESSI observations (positions of X-ray sources) with Phoenix-2 data (identification of radio spikes) and observations from the Nancay Radio Heliograph (locations of the radio emission in 4 discrete frequencies) in a particularly well observed limb event we can find - at least one - answer to the above question. Figure one shows the radio spectrogram and the thermal and nonthermal X-ray light curves of the event. The spikes occured in the impulsive phase, when the soft X-ray emission was still rising. However, the radio emission is not clearly correlated with the details of the hard X-ray lightcurve.  
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[[Image:Mb_spikelcurve.jpg|650px|thumb|center|'''Figure 1''' (left): "Top": Phoenix-2 spectrogram. Narrowband radio spikes occurred during most of the displayed time, but two distinct intervals can be distinguished delimited by white vertical lines in the spectrogram. "Bottom": RHESSI light curves of nonthermal emission and GOES light curve of the 1-8 <math>\AA</math> band produced by thermal emission.]]
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[[Image:Mb_spikeposition.jpg|650px|thumb|center|'''Figure 1''' (left): An MDI line-of-sight magnetogram of active region no. 10465.  RHESSI microflare locations are marked by crosses and are seemingly not evenly distributed but accumulate in complex magnetic regions. The bottom panel shows the same region in white light (TRACE) where we see sunspots. <br>'''Figure 2''' (right): The time evolution of one of these microflares (GOES A5) observed in the corona (T~1 MK) and the chromosphere (T~ 7,000 K). Features expected from the flare cartoons are obvious (e.g. chromospheric flare loop footpoints with a hot X-ray loop lying in between, as well as a postflare loop). The RHESSI loop ends are located in areas of opposite polarity.]]
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Now let us have a look at the spatial relations.  
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[[Image:Mb_spikeposition.jpg|650px|thumb|center|'''Figure 2''' (left): An MDI line-of-sight magnetogram of active region no. 10465.  RHESSI microflare locations are marked by crosses and are seemingly not evenly distributed but accumulate in complex magnetic regions. The bottom panel shows the same region in white light (TRACE) where we see sunspots. <br>'''Figure 2''' (right): The time evolution of one of these microflares (GOES A5) observed in the corona (T~1 MK) and the chromosphere (T~ 7,000 K). Features expected from the flare cartoons are obvious (e.g. chromospheric flare loop footpoints with a hot X-ray loop lying in between, as well as a postflare loop). The RHESSI loop ends are located in areas of opposite polarity.]]
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[[Image:Mb_spikeposition.jpg|650px|thumb|center|'''Figure 2''' (left): The geometry observed for the two intervals defined in Fig. 1. RHESSI contours of the hard X-ray "coronal" sources at 18-22 keV are shown in <span style="color:#00BFFF"> light blue </span> and at 6-12 keV (thermal) in <span style="color:#FF0000"> red</span>. "Footpoint" sources at 25-50 keV are shown in <span style="color:#00008B"> dark blue</span> ]]
'''Biographical Note:''' Arnold Benz is Professor at ETH Zurich, Switzerland. Marina Battaglia ist a post-doctoral research fellow at the University of Glasgow, Scotland.
'''Biographical Note:''' Arnold Benz is Professor at ETH Zurich, Switzerland. Marina Battaglia ist a post-doctoral research fellow at the University of Glasgow, Scotland.

Revision as of 13:25, 8 June 2009

Introduction

In the standard solar flare scenario, a large number of particles (electrons and protons) are accelerated in the solar corona. Radiative signatures of those particles are found in X-rays and radio wavelenghts, teling us the the particles are non-thermally distributed in energy. Assuming that the same distribution of particles causes both, X-ray and radio emission, one would expect a close relation of the two emission types. Indeed, millisecond spikes have been found to have a high temporal association rate with hard X-rays.

But what about the spatial relations? Sticking to the picture of a coronal acceleration site one would expect coronal X-ray emission and radio spikes to originate from the same positions.

Observations

By combining RHESSI observations (positions of X-ray sources) with Phoenix-2 data (identification of radio spikes) and observations from the Nancay Radio Heliograph (locations of the radio emission in 4 discrete frequencies) in a particularly well observed limb event we can find - at least one - answer to the above question. Figure one shows the radio spectrogram and the thermal and nonthermal X-ray light curves of the event. The spikes occured in the impulsive phase, when the soft X-ray emission was still rising. However, the radio emission is not clearly correlated with the details of the hard X-ray lightcurve.

Figure 1 (left): "Top": Phoenix-2 spectrogram. Narrowband radio spikes occurred during most of the displayed time, but two distinct intervals can be distinguished delimited by white vertical lines in the spectrogram. "Bottom": RHESSI light curves of nonthermal emission and GOES light curve of the 1-8 \AA band produced by thermal emission.

Now let us have a look at the spatial relations.

Figure 2 (left): The geometry observed for the two intervals defined in Fig. 1. RHESSI contours of the hard X-ray "coronal" sources at 18-22 keV are shown in light blue and at 6-12 keV (thermal) in red. "Footpoint" sources at 25-50 keV are shown in dark blue


Biographical Note: Arnold Benz is Professor at ETH Zurich, Switzerland. Marina Battaglia ist a post-doctoral research fellow at the University of Glasgow, Scotland.

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