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The energy of waves in the photosphere and lower chromosphere: IV. Inversion results of Ca II H spectra
Solar and Stellar Astrophysics · Submitted 27 Feb 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The large difference between QS regions and ARs, and the better match of AR and non-LTE reference spectra suggest that magnetic heating processes are more important than commonly assumed.
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The abstract, sentence by sentence
Most static 1D atmosphere models in the quiet Sun predict a rise of the gas temperature at chromospheric layers, but numerical simulations only yield an increase in the brightness temperature. We investigate the thermal structure in the solar chromosphere as derived from an LTE inversion of Ca II H spectra in QS and active regions. We investigate the temperature stratifications on differences between magnetic and field-free regions in the QS, and between QS and ARs. We determine the energy content of individual calcium bright grains (BGs). The rms temperature fluctuations are below 100 K in the photosphere and 200-300 K in the chromosphere. The average temperature stratification in the QS does not exhibit a clear chromospheric temperature rise, opposite to the AR case. We find an energy content of about 7*10E18 J for BGs that repeat with a cadence of about 160 secs. The precursors of BGs have a vertical extent of about 200 km and a horizontal extent of about 1 Mm. The comparison of observed with synthetic NLTE profiles confirms that the solar chromosphere in the QS oscillates between an atmosphere in radiative equilibrium and one with a moderate chromospheric temperature rise. Two-dimensional x-z temperature maps exhibit nearly horizontal canopy-like structures with a few Mm extent around photospheric magnetic field concentrations at a height of about 600 km. The large difference between QS regions and ARs, and the better match of AR and non-LTE reference spectra suggest that magnetic heating processes are more important than commonly assumed. The temperature fluctuations in QS derived by the LTE inversion do not suffice on average to maintain a stationary chromospheric temperature rise. The spatially and vertically resolved information on the temperature structure allows one to investigate in detail the topology and evolution of the thermal structure in the lower solar atmosphere.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Most static 1D atmosphere models in the quiet Sun predict a rise of the gas temperature at chromospheric layers, but numerical simulations only yield an increase in the brightness temperature. | background 0.95 | 0.05 | 0.05 | asserted 1.00 |
| s1 | We investigate the thermal structure in the solar chromosphere as derived from an LTE inversion of Ca II H spectra in QS and active regions. | contribution 0.89 | 0.93 | 0.04 | asserted 0.76 |
| s2 | We investigate the temperature stratifications on differences between magnetic and field-free regions in the QS, and between QS and ARs. | contribution 0.99 | 0.87 | 0.04 | asserted 0.50 |
| s3 | We determine the energy content of individual calcium bright grains (BGs). | contribution 0.96 | 0.94 | 0.04 | asserted 0.91 |
| s4 | The rms temperature fluctuations are below 100 K in the photosphere and 200-300 K in the chromosphere. | result 1.00 | 0.89 | 0.08 | asserted 1.00 |
| s5 | The average temperature stratification in the QS does not exhibit a clear chromospheric temperature rise, opposite to the AR case. | result 1.00 | 0.90 | 0.24 | asserted 1.00 |
| s6 | We find an energy content of about 7*10E18 J for BGs that repeat with a cadence of about 160 secs. | result 1.00 | 0.96 | 0.08 | asserted 1.00 |
| s7 | The precursors of BGs have a vertical extent of about 200 km and a horizontal extent of about 1 Mm. | result 1.00 | 0.89 | 0.03 | asserted 1.00 |
| s8 | The comparison of observed with synthetic NLTE profiles confirms that the solar chromosphere in the QS oscillates between an atmosphere in radiative equilibrium and one with a moderate chromospheric temperature rise. | result 0.94 | 0.86 | 0.25 | asserted 0.99 |
| s9 | Two-dimensional x-z temperature maps exhibit nearly horizontal canopy-like structures with a few Mm extent around photospheric magnetic field concentrations at a height of about 600 km. | result 1.00 | 0.90 | 0.06 | asserted 1.00 |
| s10 | The large difference between QS regions and ARs, and the better match of AR and non-LTE reference spectra suggest that magnetic heating processes are more important than commonly assumed. | interpretation 1.00 | 0.87 | 0.59 | hedged possibility 0.97 |
| s11 | The temperature fluctuations in QS derived by the LTE inversion do not suffice on average to maintain a stationary chromospheric temperature rise. | result 0.56 | 0.94 | 0.27 | asserted 0.99 |
| s12 | The spatially and vertically resolved information on the temperature structure allows one to investigate in detail the topology and evolution of the thermal structure in the lower solar atmosphere. | interpretation 0.37 | 0.47 | 0.07 | asserted 0.63 |
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Original abstract
Most static 1D atmosphere models in the quiet Sun predict a rise of the gas temperature at chromospheric layers, but numerical simulations only yield an increase in the brightness temperature. We investigate the thermal structure in the solar chromosphere as derived from an LTE inversion of Ca II H spectra in QS and active regions. We investigate the temperature stratifications on differences between magnetic and field-free regions in the QS, and between QS and ARs. We determine the energy content of individual calcium bright grains (BGs). The rms temperature fluctuations are below 100 K in the photosphere and 200-300 K in the chromosphere. The average temperature stratification in the QS does not exhibit a clear chromospheric temperature rise, opposite to the AR case. We find an energy content of about 7*10E18 J for BGs that repeat with a cadence of about 160 secs. The precursors of BGs have a vertical extent of about 200 km and a horizontal extent of about 1 Mm. The comparison of observed with synthetic NLTE profiles confirms that the solar chromosphere in the QS oscillates between an atmosphere in radiative equilibrium and one with a moderate chromospheric temperature rise. Two-dimensional x-z temperature maps exhibit nearly horizontal canopy-like structures with a few Mm extent around photospheric magnetic field concentrations at a height of about 600 km. The large difference between QS regions and ARs, and the better match of AR and non-LTE reference spectra suggest that magnetic heating processes are more important than commonly assumed. The temperature fluctuations in QS derived by the LTE inversion do not suffice on average to maintain a stationary chromospheric temperature rise. The spatially and vertically resolved information on the temperature structure allows one to investigate in detail the topology and evolution of the thermal structure in the lower solar atmosphere.
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