This looks very nice.  Can you rule out any heating mechanisms?  Is the 
really hot stuff (in)consistent with the emergence and dissipation of new magnetic field from below via a long-lived reconnection due to the underlying continuous emergence of flux?



On Thu, Jul 27, 2017 at 3:18 AM, Susanna Parenti <susanna.parenti@ias.u-psud.fr> wrote:
Dear all,
 
  here is a new paper just accepted for publication on the ApJ. It provides evidence for very hot plasma above the limb observed for an AR using spectroscopic observations from Fe X to Fe XIX.  We quantify the spatial and temporal properties of this plasma. Main results: the hot plasma is detected in various places above the limb which are at different heights; its thermal properties are not changing much over the duration of the observations (17h) .

Regards,

Susanna Parenti


http://arxiv.org/abs/1707.08445

Spectroscopy of very hot plasma in non-flaring parts of a solar limb active region: spatial and temporal properties.

In this work we investigate the thermal structure of an off-limb active region in various non-flaring areas, as it provides key information on the way these structures are heated. In particular, we concentrate in the very hot component (>3 MK) as it is a crucial element to discriminate between different heating mechanisms. We present an analysis using Fe and Ca emission lines from both SOHO/SUMER and HINODE/EIS. A dataset covering all ionization stages from Fe X to Fe XIX has been used for the thermal analysis (both DEM and EM). Ca XIV is used for the SUMER-EIS radiometric cross-calibration. We show how the very hot plasma is present and persistent almost everywhere in the core of the limb AR. The off-limb AR is clearly structured in Fe XVIII. Almost everywhere, the EM analysis reveals plasma at 10 MK (visible in Fe XIX emission) which is down to 0.1% of EM of the main 3 MK plasma. We estimate the power law index of the hot tail of the EM to be between -8.5 and -4.4. However, we leave an open question on the possible existence of a small minor peak at around 10 MK. The absence in some part of the AR of Fe XIX and Fe XXIII lines (which fall into our spectral range) enables us to determine an upper limit on the EM at such temperatures. Our results include a new Ca XIV 943.59 \AA~ atomic model



 

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