Abstract <p>We observed a B6.2-class solar flare in active region NOAA 12651 using the HSFA spectrograph at the Ondřejov Observatory in hydrogen spectral lines. After processing the spectra, the integral emission fluxes in the H<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8819_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha\)</EquationSource> <!--BPhysMGU2570070Kupryakov-m1--> </InlineEquation>, H<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8819_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\beta\)</EquationSource> <!--BPhysMGU2570070Kupryakov-m2--> </InlineEquation>, and H<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8819_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon\)</EquationSource> <!--BPhysMGU2570070Kupryakov-m3--> </InlineEquation> lines were determined. Within the heated-gas approach, a theoretical reconstruction of the plasma parameters was performed, taking into account the physical conditions in the chromosphere, including self-absorption in the spectral lines. Treating the observed fluxes requires the assumption of inhomogeneous gas. Agreement between the theoretical and observed fluxes is achieved in a model involving the superposition of two gas layers. Behind lies a dense gas with concentration <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8819_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(N\)</EquationSource> <!--BPhysMGU2570070Kupryakov-m4--> </InlineEquation> ranging from <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8819_Article_IEq5.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(3\times 10^{12}\)</EquationSource> <!--BPhysMGU2570070Kupryakov-m5--> </InlineEquation> to <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8819_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(3\times 10^{13}\)</EquationSource> <!--BPhysMGU2570070Kupryakov-m6--> </InlineEquation> cm<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8819_Article_IEq7.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{-3}\)</EquationSource> <!--BPhysMGU2570070Kupryakov-m7--> </InlineEquation>, and between it and the observer is a rarefied layer where <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8819_Article_IEq8.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="129" /> </InlineMediaObject> <EquationSource Format="TEX">\(N=(3{-}6)\times 10^{10}\)</EquationSource> <!--BPhysMGU2570070Kupryakov-m8--> </InlineEquation> cm<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8819_Article_IEq7.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{-3}\)</EquationSource> <!--BPhysMGU2570070Kupryakov-m9--> </InlineEquation>. The layer thickness is in the range from 600 to 3000 km, the temperature—between 4000 and 7200 K, and the turbulent velocity—from 0 to 90 km/s. The presence of dense regions indicates that the source of the observed emission originates from the middle chromosphere, not higher than 1000 km.</p>

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Analysis of Balmer Series Emission in the Solar Flare SOL2017-04-21

  • Yu. A. Kupryakov,
  • V. A. Maliutin,
  • K. V. Bychkov,
  • A. B. Gorshkov,
  • O. M. Belova

摘要

Abstract

We observed a B6.2-class solar flare in active region NOAA 12651 using the HSFA spectrograph at the Ondřejov Observatory in hydrogen spectral lines. After processing the spectra, the integral emission fluxes in the H \(\alpha\) , H \(\beta\) , and H \(\varepsilon\) lines were determined. Within the heated-gas approach, a theoretical reconstruction of the plasma parameters was performed, taking into account the physical conditions in the chromosphere, including self-absorption in the spectral lines. Treating the observed fluxes requires the assumption of inhomogeneous gas. Agreement between the theoretical and observed fluxes is achieved in a model involving the superposition of two gas layers. Behind lies a dense gas with concentration \(N\) ranging from \(3\times 10^{12}\) to \(3\times 10^{13}\) cm \({}^{-3}\) , and between it and the observer is a rarefied layer where \(N=(3{-}6)\times 10^{10}\) cm \({}^{-3}\) . The layer thickness is in the range from 600 to 3000 km, the temperature—between 4000 and 7200 K, and the turbulent velocity—from 0 to 90 km/s. The presence of dense regions indicates that the source of the observed emission originates from the middle chromosphere, not higher than 1000 km.