4.6 Article

Active region moss Basic physical parameters and their temporal variation

Journal

ASTRONOMY & ASTROPHYSICS
Volume 518, Issue -, Pages -

Publisher

EDP SCIENCES S A
DOI: 10.1051/0004-6361/200913883

Keywords

Sun: atmosphere; Sun: activity; Sun: corona; Sun: UV radiation; Sun: transition region; Sun: magnetic topology

Funding

  1. STFC
  2. Hinode/EIS team
  3. STFC [PP/E004857/2, ST/G002584/1, ST/H000429/1, PP/D002907/1] Funding Source: UKRI
  4. Science and Technology Facilities Council [PP/E004857/2, ST/G002584/1, ST/H000429/1, PP/D002907/1] Funding Source: researchfish

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Context. Active region moss are transition region phenomena, first noted in the images recorded by the Transition Region and Coronal Explorer (TRACE) in lambda 171. Moss regions are thought to be the footpoints of hot loops (3-5 MK) seen in the core of active regions. These hot loops appear fuzzy (unresolved). Therefore, it is difficult to study the physical plasma parameters in individual hot core loops and hence their heating mechanisms. Moss regions provide an excellent opportunity to study the physics of hot loops. In addition, they allow us to study the transition region dynamics in the footpoint regions. Aims. To derive the physical plasma parameters such as temperature, electron density, and filling factors in moss regions and to study their variation over a short (an hour) and a long time period (5 consecutive days). Methods. Primarily, we have analyzed spectroscopic observations recorded by the Extreme-ultraviolet Imaging Spectrometer (EIS) aboard Hinode. In addition we have used supplementary observations taken from TRACE and the X-Ray Telescope (XRT) aboard Hinode. Results. The moss emission is strongest in the Fe XII and Fe XIII lines. Based on analyses using line ratios and emission measure we found that moss regions have a characteristic temperature of log T[K] = 6.2. The temperature structure in moss region remains almost identical from one region to another and it does not change with time. The electron densities measured at different locations in the moss regions using Fe XII ratios are about 1-3x10(10) cm(-3) and about 2-4x10(9) cm(-3) using Fe XIII and Fe XIV The densities in the moss regions are similar in different places and show very little variation over short and long time scales. The derived electron density substantially increased (by a factor of about 3-4 or even more in some cases) when a background subtraction was performed. The filling factor of the moss plasma can vary between 0.1-1 and the path length along which the emission originates is from a few 100 to a few 1000 kms long. By combining the observations recorded by TRACE, EIS and XRT, we find that the moss regions correspond to the footpoints of both hot and warm loops.

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