Calculated brightness temperatures of solar structures compared with ALMA and Metsähovi measurements

Author:

Matković Filip1ORCID,Brajša Roman1,Kuhar Matej23,Benz Arnold O.24,Ludwig Hans ‐G.5,Selhorst Caius L.67,Skokić Ivica1,Sudar Davor1,Hanslmeier Arnold8

Affiliation:

1. Hvar Observatory, Faculty of Geodesy University of Zagreb Zagreb Croatia

2. Institute for Data Science University of Applied Sciences and Arts Northwestern Switzerland Windisch Switzerland

3. Finstar, c/o Hypothekarbank Lenzburg AG Lenzburg Switzerland

4. Institute for Particle Physics and Astrophysics Department of Physics, ETH Zurich Zurich Switzerland

5. Landessternwarte Königstuhl Zentrum für Astronomie der Universität Heidelberg Heidelberg Germany

6. NAT ‐ Núcleo de Astrofísica, Universidade Cidade de São Paulo São Paulo Brazil

7. Center for Solar‐Terrestrial Research New Jersey Institute of Technology Newark New Jersey USA

8. Institute for Geophysics, Astrophysics and Meteorology Institute of Physics, University of Graz Graz Austria

Abstract

AbstractThe Atacama Large Millimeter/submillimeter Array (ALMA) allows for solar observations in the wavelength range of 0.3–10 mm, giving us a new view of the chromosphere. The measured brightness temperature at various frequencies can be fitted with theoretical models of density and temperature versus height. We use the available ALMA and Metsähovi measurements of selected solar structures (quiet sun (QS), active regions (AR) devoid of sunspots, and coronal holes (CH)). The measured QS brightness temperature in the ALMA wavelength range agrees well with the predictions of the semiempirical Avrett–Tian–Landi–Curdt–Wülser (ATLCW) model, better than previous models such as the Avrett–Loeser (AL) or Fontenla–Avrett–Loeser model (FAL). We scaled the ATLCW model in density and temperature to fit the observations of the other structures. For ARs, the fitted models require 9%–13% higher electron densities and 9%–10% higher electron temperatures, consistent with expectations. The CH fitted models require electron densities 2%–40% lower than the QS level, while the predicted electron temperatures, although somewhat lower, do not deviate significantly from the QS model. Despite the limitations of the one‐dimensional ATLCW model, we confirm that this model and its appropriate adaptations are sufficient for describing the basic physical properties of the solar structures.

Funder

Alexander von Humboldt Foundation

Hrvatska Zaklada za Znanost

Deutsche Forschungsgemeinschaft

Centros de Pesquisa, Inovação e Difusão, Fundação Amazônia Paraense de Amparo à Pesquisa

Publisher

Wiley

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