Bibcode
Franz, M.; Collados, M.; Bethge, C.; Schlichenmaier, R.; Borrero, J. M.; Schmidt, W.; Lagg, A.; Solanki, S. K.; Berkefeld, T.; Kiess, C.; Rezaei, R.; Schmidt, D.; Sigwarth, M.; Soltau, D.; Volkmer, R.; von der Luhe, O.; Waldmann, T.; Orozco, D.; Pastor Yabar, A.; Denker, C.; Balthasar, H.; Staude, J.; Hofmann, A.; Strassmeier, K.; Feller, A.; Nicklas, H.; Kneer, F.; Sobotka, M.
Bibliographical reference
Astronomy and Astrophysics, Volume 596, id.A4, 13 pp.
Advertised on:
11
2016
Journal
Citations
24
Refereed citations
23
Description
Context. A significant part of the penumbral magnetic field returns
below the surface in the very deep photosphere. For lines in the
visible, a large portion of this return field can only be detected
indirectly by studying its imprints on strongly asymmetric and
three-lobed Stokes V profiles. Infrared lines probe a narrow layer in
the very deep photosphere, providing the possibility of directly
measuring the orientation of magnetic fields close to the solar surface.
Aims: We study the topology of the penumbral magnetic field in
the lower photosphere, focusing on regions where it returns below the
surface. Methods: We analyzed 71 spectropolarimetric datasets
from Hinode and from the GREGOR infrared spectrograph. We inferred the
quality and polarimetric accuracy of the infrared data after applying
several reduction steps. Techniques of spectral inversion and forward
synthesis were used to test the detection algorithm. We compared the
morphology and the fractional penumbral area covered by
reversed-polarity and three-lobed Stokes V profiles for sunspots at disk
center. We determined the amount of reversed-polarity and three-lobed
Stokes V profiles in visible and infrared data of sunspots at various
heliocentric angles. From the results, we computed center-to-limb
variation curves, which were interpreted in the context of existing
penumbral models. Results: Observations in visible and
near-infrared spectral lines yield a significant difference in the
penumbral area covered by magnetic fields of opposite polarity. In the
infrared, the number of reversed-polarity Stokes V profiles is smaller
by a factor of two than in the visible. For three-lobed Stokes V
profiles the numbers differ by up to an order of magnitude.