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Expanding Magnetic Canopy Structure and Parasitic Polarities in a Quiet-Sun Network Element Observed by SUNRISE III/SCIP

  • Authors: Ryan J. Campbell, Carlos Quintero Noda, Mihalis Mathioudakis, Manuel Collados, Jack McFall, David B. Jess, Sami K. Solanki, Andreas Lagg, Achim Gandorfer, Jose Carlos del Toro Iniesta, Yukio Katsukawa, Pietro Bernasconi, Thomas Berkefeld, Alex Feller, Tino L. Riethmüller, Alberto Álvarez-Herrero, Masahito Kubo, H. N. Smitha, David Orozco Suárez, Bianca Grauf, Michael Carpenter, Alexander Bell, Valentín Martínez Pillet, Francisco Javier Bailén, Julian Blanco Rodríguez, Juan Sebastián Castellanos Durán, Edvarda Harnes, Johannes Hölken, Francisco A. Iglesias, Ryohtaroh T. Ishikawa, Yusuke Kawabata, Takuma Matsumoto, Takayoshi Oba, Azaymi L. Siu-Tapia, Hanna Strecker, Dušan Vukadinović, Hirohisa Hara, Toshifumi Shimizu

Ryan J. Campbell et al 2026 The Astrophysical Journal Letters 1008 .

  • Provider: AAS Journals

Caption: Figure 1.

Overview of the analyzed network region and corresponding depth-dependent magnetic structure along three selected cuts. Top row: continuum intensity (left), maximum linear polarization signal ﹩{{\rm{\max }}}_{\lambda }\sqrt{{Q}^{2}+{U}^{2}}﹩ (middle), and Stokes V in the Fe I 8468 Å wing (right). Three spatial cuts (A, B, and C) tracing the linear polarization ridge are taken. Lower panels: stratifications along cuts A–C as a function of distance and optical depth ﹩\mathrm{log}\tau ﹩. Rows show LOS magnetic field BLOS, total field strength Btot, and transverse field component B, respectively. The dashed red box highlights the region shown in Figure 2. All Stokes quantities are continuum normalized. The tick marks on the upper panels and vertical lines on the lower panels denote 1″ increments. The median values at given optical depths are indicated on the bottom panels.

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