Solar plage regions — patches of concentrated magnetic field where hot coronal loops root — have well-measured photospheric fields but poorly known chromospheric fields, and the mechanism that heats the plage chromosphere is unresolved. High-sensitivity spectropolarimetry with the Daniel K. Inouye Solar Telescope's Visible Spectro-Polarimeter (DKIST/ViSP) (da Silva Santos et al. 2023) measured ‘∼‘`\sim`200–300 G fields in plage fibrils, found a clear field-strength/λ8542\lambda8542-emission correlation over the whole field of view that weakens inside plage, and detected supersonic downflows at the plage periphery, but could not determine how the field expands with height, whether the Ca II 8542 Å line quantitatively traces chromospheric cooling rates, or whether current systems at flux-tube edges cause the observed localized heating. The open problem is to establish the three-dimensional structure of the plage chromospheric magnetic field — its weakening and expansion with height, measured systematically across heliocentric angles and plage samples — together with the three-dimensional distribution of radiative cooling rates in the lower chromosphere, and to determine whether the magnetic topology (including edge-localized currents, i.e. the curl of B\mathbf{B}) causally shapes the heating, including the origin of the peripheral supersonic downflows.

Background

Plage regions are patches of strong, predominantly unipolar magnetic field in the solar photosphere, seen in chromospheric diagnostics as bright Ca II emission; they are the footpoint regions of hot coronal loops. The chromosphere — the ‘∼‘`\sim`10,000 K layer between the photosphere and the corona — is heated by mechanisms that remain unidentified, and in plage the heating is known to be magnetic in origin. Spectropolarimetry measures the four Stokes parameters (II, intensity; QQ, UU, linear polarization; VV, circular polarization) of a spectral line; the Ca II 8542 Å line (λ8542\lambda8542, of the infrared Ca II triplet) forms in the low-to-middle chromosphere and is sensitive to magnetic fields through the Zeeman effect. Because its polarization signals are weak, plage chromospheric fields are commonly inferred with the weak-field approximation (WFA, a linear relation between Stokes VV and the line-of-sight field valid for weak fields) or with Milne–Eddington (ME) inversions, which assume a simplified one-component atmosphere; full non-local thermodynamic equilibrium (NLTE) inversions retrieve height-resolved atmosphere models by fitting the line formation physics. The magnetic canopy is the fan of expanding, highly inclined field lines spreading from photospheric flux concentrations and traced by dark fibrils in chromospheric images.

Photospheric plage fields are strong (kilogauss) and well characterized, but chromospheric values were scarce before DKIST: spatially-regularized WFA applied to Swedish 1-m Solar Telescope data found canopy field stratification over one plage (Morosin et al. 2020), and CLASP2 (the Chromospheric Lyman-Alpha Spectro-Polarimeter sounding-rocket experiment, second flight) spectropolarimetry of the Mg II h and k lines mapped longitudinal fields from the photosphere to the upper chromosphere in active regions (Ishikawa et al. 2021). Semi-empirical models established that the Ca II lines dominate chromospheric radiative losses (Vernazza, Avrett & Loeser 1981), and observations show enhanced λ8542\lambda8542 emission near magnetic elements, offset from the strongest fields — interpreted as resistive heating at the edges of flux tubes (de la Cruz Rodríguez et al. 2013) — while NLTE inversions of one plage found heating concentrated away from the field maxima (Morosin et al. 2022). Co-spatial Ca II K / Ca II 8542 spectropolarimetry of one active-region plage has since established the height expansion directly (Juanikorena Berasategi et al. 2026), confirming the effect qualitatively for a single region but not supplying the systematic multi-region, multi-heliocentric-angle sampling needed to separate viewing-angle effects from intrinsic field geometry.

The source paper (da Silva Santos et al. 2023) used the Daniel K. Inouye Solar Telescope (DKIST) Visible Spectro-Polarimeter (ViSP) to observe one extended, decaying plage with ‘∼‘`\sim`2 G noise. It found ‘∼‘`\sim`200–300 G total fields in fibrils, an average line-of-sight chromospheric field of ∼\sim-210 G, a clear field-strength/cooling-proxy correlation over the whole field of view that weakens inside plage, and supersonic (‘∼‘`\sim`15 km s−1^{-1}) downflows at the plage periphery. Its conclusions state what remains open: the height expansion of the plage magnetic field (requiring a larger sample and a range of heliocentric angles μ\mu, the cosine of the viewing angle, to separate viewing effects from intrinsic geometry), the three-dimensional distribution of heating rates (the source notes that if heating is resistive at flux-tube edges, emission should correlate with the curl of B\mathbf{B} — the electric current density — rather than with B\mathbf{B} itself), whether λ8542\lambda8542 integrated intensity quantitatively traces the radiative cooling rates in plage, the origin and energetics of the supersonic downflows, and — as enabling capabilities — improved λ8542\lambda8542-arm calibration, NLTE multi-line inversions, and extended chromospheric magnetograms suitable for extrapolating fields into the corona and heliosphere for comparison with in situ Parker Solar Probe measurements.

Problem Statement

Establish the three-dimensional structure of the plage chromospheric magnetic field and its causal relationship to localized chromospheric heating. Concretely, for solar plage regions: (i) measure how the magnetic field weakens and expands with height from the kilogauss photospheric concentrations through the chromospheric canopy, systematically over a sample of plage regions and a range of heliocentric angles μ\mu (the cosine of the angle between the line of sight and the local solar vertical), so that viewing-angle effects are separated from intrinsic field geometry; (ii) determine the three-dimensional distribution of radiative cooling rates in the lower chromosphere of plage and quantify whether Ca II 8542 Å integrated intensity is a faithful proxy for those rates; (iii) establish or exclude a causal link between the magnetic topology and the localized heating — in particular whether enhanced λ8542\lambda8542 emission at flux-tube edges is produced by resistive heating associated with edge currents, i.e. whether it correlates with the curl of B\mathbf{B} rather than with the field strength B\mathbf{B} itself; and (iv) as part of the plage dynamics this structure governs, determine the origin (draining of cold material, shock formation, or reconnection outflows) and energetic significance of the supersonic (‘∼‘`\sim`15 km s−1^{-1}) downflows at plage peripheries. These four components are all required and jointly answer one question — what is the 3D magnetic structure of plage and does that structure cause the observed chromospheric heating? — with improved λ8542\lambda8542 calibration, NLTE multi-line inversions, and extended chromospheric magnetograms serving as the means that enable it.

References

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