Submit manuscript...
eISSN: 2576-4543

Physics & Astronomy International Journal

Mini Review Volume 1 Issue 4

Time series of solar coronal bright point

Javaherian M, Kaki B, Mehrabian M

Department of Physics, University of Zanjan, Iran

Correspondence: Mohsen Javaherian, Department of Physics, University of Zanjan, P.O. Box 45195-313, Zanjan, Iran

Received: October 03, 2017 | Published: October 17, 2017

Citation: Javaherian M, Kaki B, Mehrabian M, et al. Time series of solar coronal bright point. Phys Astron Int J. 2017;1(4):123-124. DOI: 10.15406/paij.2017.01.00022

Download PDF

Abstract

The solar corona is covered by coronal bright points (CBPs) which are observable features in X-ray and extreme ultra violet wavelengths. Since statistical properties of BPs (e.g., size, lifetime) play important role in solar coronal evolution, lots of automatic detection methods and pattern recognition approaches were developed to detect (e.g., region growing function) and track these magnetic structures all over the corona. CBPs are appeared as different morphological structures such as point-like, small-loop, and small active regions in the corona. The properties of BPs can be contained important information about coronal heating. Here, we want to review some significant characteristics of BPs and give an outline about our idea to work with the time series of coronal BPs.

Keywords: Sun, corona, Sun, bright point (BP), Technique, region growing

Introduction

The solar corona is the origin of many phenomena having a profound effect in space weather and interstellar medium. Historically, the corona is divided into three main regions: active region (AR), quiet Sun (QS), and coronal hole (CH).1 Coronal bright points (CBPs), which are firstly observed in X-ray and extreme ultraviolet solar images (Figure 1, left panel) and discussed in,2,3 are emerged in quiet-Sun regions and coronal holes. Typically, these bright features have lifetimes and sizes less than an hour and 60 arcsec, respectively.3

The appearance of CBPs can return to the configuration of magnetic flux and canceling of magnetic bipoles.4,5Nowadays, by increasing received data from the Sun with high- temporal and spatial resolution space-borne and ground-based instruments established, the needs for using automatic detections and pattern recognition approaches has increased.610

One of the important problems about the Sun is coronal heating that can be related to CBPs and nano-flares.11 Studying statistical CBPs can reveal some characteristics of solar activity.12 Presented lots of important statistical properties of CBPs from EUV images taken by Solar Dynamic Observatory (SDO)/ Atmospheric Imaging Assembly (AIA)13 using automatic detection methods.

The basic procedure of work

Here, we cropped a part of full disc solar image including a CBP over sequential EUV images taken at 171Å recorded by SDO/AIA. Then, the region growing function was applied to the cropped images to segregate CBP in all consecutive images (Figure 1, right panel). The time cadence between two consecutive images is 12s. The mean intensity of this segmented feature was extracted as light curves (Figure 2). A sample of CBP time series (points) with a fitting of Gaussian function (blue line) are shown in Figure 2.

Figure 1 A cropped part of EUV image including a CBP recorded by SDO/AIA (left panel) taken at 171Å. A segmented image representing CBP (right panel).

Figure 2 The extracted normalized mean intensity of one CBP (shown in Figure 1) over its lifetime in sequential EUV images with a time lag 12s. By applying a Gaussian fit, f( x )=a e ( ( xb )/c ) 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfaieaaaaaa aaa8qacaWGMbWaaeWaa8aabaWdbiaadIhaaiaawIcacaGLPaaacqGH 9aqpcaWGHbGaamyza8aadaahaaqcfasabeaajuaGpeWaaeWaaKqbG8 aabaWdbiabgkHiTKqbaoaabmaajuaipaqaa8qacaWG4bGaeyOeI0Ia amOyaaGaayjkaiaawMcaaiaac+cacaWGJbaacaGLOaGaayzkaaqcfa 4damaaCaaajuaibeqaa8qacaaIYaaaaaaaaaa@4954@ the parameters a, b and c were obtained 0.95, 15.21, and 35, respectively.

Conclusion

As it is seen in Figure 2, the rising and the decay of mean intensity of the selected CBP has been occurred over approximately 7 minutes. We applied a Gaussian fit as f( x )=a e ( ( xb )/c ) 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfaieaaaaaa aaa8qacaWGMbWaaeWaa8aabaWdbiaadIhaaiaawIcacaGLPaaacqGH 9aqpcaWGHbGaamyza8aadaahaaqabKqbGeaajuaGpeWaaeWaaKqbG8 aabaWdbiabgkHiTKqbaoaabmaajuaipaqaa8qacaWG4bGaeyOeI0Ia amOyaaGaayjkaiaawMcaaiaac+cacaWGJbaacaGLOaGaayzkaaqcfa 4damaaCaaajuaibeqaa8qacaaIYaaaaaaaaaa@4954@  to the normalized light curve of the CBP. The parameters a, b and c were obtained 0.95, 15.21, and 35, respectively, with 95% confidence. The peak of fitting shows that the brightness of CBP reached at maximum value at 3 minutes.
In the future, we aim to investigate some properties of CBPs time series, statistically, over their lifetimes. The statistical moments of CBPs (e.g., mean, variance, and skewness) may contain important information.

Acknowledgments

None.

Conflicts of interest

Authors declare that there are no conflicts of interests.

References

  1. Aschwanden MJ. Physics of the Solar Corona. 2nd ed, Praxis Publishing, Springer, Berlin, UK. 2006.
  2. Vaiana GS, Krieger AS, Van Speybroec LP,et al. BAPS 15. 1970. 611 p.
  3. Vaiana GS, Davis JM, Giacconi R, et al. X-Ray Observations of Characteristic Structures and Time Variations from the Solar Corona: Preliminary Results from SKYLAB. The Astrophysical Journal. 1973;185:47–51.
  4. Parnell CE, Priest ER, Golub L. The three-dimensional structures of X-ray bright points. Solar Physics.11994;51(1):57–74.
  5. Priest ER, Parnell CE, Martin SF. A converging flux model of an X-ray bright point and an associated canceling magnetic feature. The Astrophysical Journal. 1994;427(1):459–474.
  6. Bovelet B, Wiehr E. Multiple-Scale Pattern Recognition Applied to Faint Intergranular G-band Structures. Solar Physics. 2007;243(1):121–129.
  7. Aschwanden MJ, Lee JK, Gary GA, et al. Comparison of Five Numerical Codes for Automated Tracing of Coronal Loops. Solar Physics. 2008;248(2):359–377.
  8. Aschwanden MJ. Image Processing Techniques and Feature Recognition in Solar Physics. Solar Physics. 2010;262(2):235–275.
  9. Javaherian M, Safari H, Amiri A, et al. Automatic Method for Identifying Photospheric Bright Points and Granules Observed by Sunrise. Solar Physics. 2014;289(10):3969–3983.
  10. Arish S, Javaherian S, Safari H, et al. Extraction of Active Regions and Coronal Holes from EUV Images Using the Unsupervised Segmentation Method in the Bayesian Framework. Solar Physics. 2016;291(4):1209–224.
  11. Tajfirouze E, Safari H. Can A Nanoflare Model Of Extreme-Ultraviolet Irradiances Describe The Heating Of The Solar Corona? The Astrophysical Journal. 2012;744(2):113–124.
  12. Alipour N, Safari H. Statistical Properties of Solar Coronal Bright Points. The Astrophysical Journal. 2015;807(2):175–184.
  13. Lemen JR, Title AM, Akin DJ, et al. The Atmospheric Imaging Assembly (AIA) on the Solar Dynamics Observatory (SDO). Solar Physics. 2012;275(1-2):17–40.
Creative Commons Attribution License

©2017 Javaherian, et al. This is an open access article distributed under the terms of the, which permits unrestricted use, distribution, and build upon your work non-commercially.