Image

Fe XIV, 530.3 nm

Our expedition observed emission from the following ions in the visible and near IR wavelength range: Fe IX (435.9 nm), Fe X (637.4 nm), Fe XI (789.2 nm), Fe XIII (1074.7 nm), Fe XIV (530.3 nm) and Ni XV (670.2 nm). These emission lines provide an excellent diagnostic tool for probing the physics of the solar corona. One of the tools is clear from the following graph. Fe XIV line at 530.3 nm is the most prominent emission line in the visible part of the coronal spectrum.
 

Even though Fe XIV is the strongest emission line in the visible part of the coronal spectrum it is not easy to obtain an image of Fe XIV only. It is not as simple as deep sky photography of emission nebulae where only sufficiently narrow band filter is needed to isolate the emission line. The light of solar corona is dominated by continuum - photospheric light scattered on free electrons. The light emitted by different atoms and ions is very weak relative to the continuum. See the following two unprocessed images. The left one was taken through a narrow band filter (bandwidth 0.5 nm) with the transmission band centered on the Fe XIV 530.3 nm emission line. The right image was taken through a filter with the transmission band outside the Fe XIV line in the continuum. It is clearly visible that except for the active region (9 o'clock position) the left image is dominated by continuum which is stronger than Fe XIV emission nearly everywhere in the image. It is not advisable to use a filter with a narrower band of transmission because the emission line is thermally broadened. Hence, a narrower band filter would make the situation even worse. Therefore it is necessary to make a precise photometric calibration of all images and than subtract the continuum - the right image from the left one. You may see these two images as an animation.
 

 
It is obvious that imaging in Fe XIV at 530.3 nm through any narrow band filter without continuum subtraction is misleading because the image is strongly dominated by continuum. If the bandwidth of the filter is wider than about 5 nm the image is nearly identical to the broadband white-light image taken without any filter. From the point of contamination by continuum Fe XIV 503.3 nm it is the worst emission line in solar corona because its wavelength is very near the maximum of the solar photospheric irradiance. On the other hand Fe XIV ions are strongly excited by photospheric light and therefore the Fe XIV emission is observable very far from the Sun. It is clearly visible if you compare the Fe XIV image presented on this page with the Fe XIII image at 1074.7 nm where the intensity of continuum relative to 530.3 nm is approximately 3× weaker.
 
More images of Fe ion emission obtained during the 2017 eclipse can be found in the following pages:
Click on the image or on the following reference to display the higher resolution image version (997 KB, PNG format).

ImageFe_XIV_Mitchell_ACHF.jpg
Date21. 08. 2017
Time2nd contact 17:21:11 UT, 3rd contact 17:23:14 UT
Placenear Mitchell, Oregon, USA
CoordinateN 44° 31.539',   W 119° 54.459',  Alt. 1100 m
ConditionsClear sky but some smoke from forest fires, solar altitude 43° above horizon
Optics2× Achromat 4/300 mm equipped with following narrow band filters:
  On-band filter: Andover, center wavelength: 530.3 nm, bandwidth 0.5 nm
  Off-band filter: Andover, center wavelength: 527.3 nm, bandwidth 0.5 nm
Camera2×Atik 314L
Exposure0.05 - 6.4 s
ProcessingComposition of 64 eclipse images (32 On-band and 32 Off-band) taken with two cameras. Images were calibrated by means of dark frames and flat-fields, aligned by means of phase correlation, composed by means of LDIC 6.0 software, continuum was removed from Fe XIV emission by subtracting the Off-band images. The resulting image was processed using Corona 5.0 software in order to visualize coronal structures. The final processing was done using ACC 6.1 software.
Image processing by Miloslav Druckmüller
SoftwareAstro D3F 2.0, PhaseCorr 7.0, LDIC 6.0, Corona 5.0, Sofo ACC 6.1
Copyright© 2017 Miloslav Druckmüller, Shadia Habbal, Pavel Štarha, Judd Johnson,
    Jana Hoderová
 


Miloslav Druckmüller
Institute of Mathematics, Faculty of Mechanical Engineering
Brno University of Technology, Czech Republic
druckmuller@fme.vutbr.cz
Page last update: 26.11.2019