Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT
Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares,...
Ausführliche Beschreibung
Autor*in: |
Trottet, G. [verfasserIn] Raulin, J.-P. [verfasserIn] Mackinnon, A. [verfasserIn] Giménez de Castro, G. [verfasserIn] Simões, P. J. A. [verfasserIn] Cabezas, D. [verfasserIn] de La Luz, V. [verfasserIn] Luoni, M. [verfasserIn] Kaufmann, P. [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2015 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: Solar physics - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967, 290(2015), 10 vom: Okt., Seite 2809-2826 |
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Übergeordnetes Werk: |
volume:290 ; year:2015 ; number:10 ; month:10 ; pages:2809-2826 |
Links: |
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DOI / URN: |
10.1007/s11207-015-0782-0 |
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Katalog-ID: |
SPR017767180 |
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245 | 1 | 0 | |a Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT |
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520 | |a Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation. | ||
650 | 4 | |a Radio bursts, microwave |7 (dpeaa)DE-He213 | |
650 | 4 | |a X-ray bursts, association with flares |7 (dpeaa)DE-He213 | |
650 | 4 | |a X-ray burst, spectrum |7 (dpeaa)DE-He213 | |
650 | 4 | |a Chromosphere, models |7 (dpeaa)DE-He213 | |
650 | 4 | |a Heating, chromospheric |7 (dpeaa)DE-He213 | |
650 | 4 | |a Heating, in flares |7 (dpeaa)DE-He213 | |
700 | 1 | |a Raulin, J.-P. |e verfasserin |4 aut | |
700 | 1 | |a Mackinnon, A. |e verfasserin |4 aut | |
700 | 1 | |a Giménez de Castro, G. |e verfasserin |4 aut | |
700 | 1 | |a Simões, P. J. A. |e verfasserin |4 aut | |
700 | 1 | |a Cabezas, D. |e verfasserin |4 aut | |
700 | 1 | |a de La Luz, V. |e verfasserin |4 aut | |
700 | 1 | |a Luoni, M. |e verfasserin |4 aut | |
700 | 1 | |a Kaufmann, P. |e verfasserin |4 aut | |
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10.1007/s11207-015-0782-0 doi (DE-627)SPR017767180 (SPR)s11207-015-0782-0-e DE-627 ger DE-627 rakwb eng 530 ASE 39.51 bkl Trottet, G. verfasserin aut Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation. Radio bursts, microwave (dpeaa)DE-He213 X-ray bursts, association with flares (dpeaa)DE-He213 X-ray burst, spectrum (dpeaa)DE-He213 Chromosphere, models (dpeaa)DE-He213 Heating, chromospheric (dpeaa)DE-He213 Heating, in flares (dpeaa)DE-He213 Raulin, J.-P. verfasserin aut Mackinnon, A. verfasserin aut Giménez de Castro, G. verfasserin aut Simões, P. J. A. verfasserin aut Cabezas, D. verfasserin aut de La Luz, V. verfasserin aut Luoni, M. verfasserin aut Kaufmann, P. verfasserin aut Enthalten in Solar physics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967 290(2015), 10 vom: Okt., Seite 2809-2826 (DE-627)269019162 (DE-600)1473830-2 1573-093X nnns volume:290 year:2015 number:10 month:10 pages:2809-2826 https://dx.doi.org/10.1007/s11207-015-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 39.51 ASE AR 290 2015 10 10 2809-2826 |
spelling |
10.1007/s11207-015-0782-0 doi (DE-627)SPR017767180 (SPR)s11207-015-0782-0-e DE-627 ger DE-627 rakwb eng 530 ASE 39.51 bkl Trottet, G. verfasserin aut Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation. Radio bursts, microwave (dpeaa)DE-He213 X-ray bursts, association with flares (dpeaa)DE-He213 X-ray burst, spectrum (dpeaa)DE-He213 Chromosphere, models (dpeaa)DE-He213 Heating, chromospheric (dpeaa)DE-He213 Heating, in flares (dpeaa)DE-He213 Raulin, J.-P. verfasserin aut Mackinnon, A. verfasserin aut Giménez de Castro, G. verfasserin aut Simões, P. J. A. verfasserin aut Cabezas, D. verfasserin aut de La Luz, V. verfasserin aut Luoni, M. verfasserin aut Kaufmann, P. verfasserin aut Enthalten in Solar physics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967 290(2015), 10 vom: Okt., Seite 2809-2826 (DE-627)269019162 (DE-600)1473830-2 1573-093X nnns volume:290 year:2015 number:10 month:10 pages:2809-2826 https://dx.doi.org/10.1007/s11207-015-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 39.51 ASE AR 290 2015 10 10 2809-2826 |
allfields_unstemmed |
10.1007/s11207-015-0782-0 doi (DE-627)SPR017767180 (SPR)s11207-015-0782-0-e DE-627 ger DE-627 rakwb eng 530 ASE 39.51 bkl Trottet, G. verfasserin aut Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation. Radio bursts, microwave (dpeaa)DE-He213 X-ray bursts, association with flares (dpeaa)DE-He213 X-ray burst, spectrum (dpeaa)DE-He213 Chromosphere, models (dpeaa)DE-He213 Heating, chromospheric (dpeaa)DE-He213 Heating, in flares (dpeaa)DE-He213 Raulin, J.-P. verfasserin aut Mackinnon, A. verfasserin aut Giménez de Castro, G. verfasserin aut Simões, P. J. A. verfasserin aut Cabezas, D. verfasserin aut de La Luz, V. verfasserin aut Luoni, M. verfasserin aut Kaufmann, P. verfasserin aut Enthalten in Solar physics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967 290(2015), 10 vom: Okt., Seite 2809-2826 (DE-627)269019162 (DE-600)1473830-2 1573-093X nnns volume:290 year:2015 number:10 month:10 pages:2809-2826 https://dx.doi.org/10.1007/s11207-015-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 39.51 ASE AR 290 2015 10 10 2809-2826 |
allfieldsGer |
10.1007/s11207-015-0782-0 doi (DE-627)SPR017767180 (SPR)s11207-015-0782-0-e DE-627 ger DE-627 rakwb eng 530 ASE 39.51 bkl Trottet, G. verfasserin aut Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation. Radio bursts, microwave (dpeaa)DE-He213 X-ray bursts, association with flares (dpeaa)DE-He213 X-ray burst, spectrum (dpeaa)DE-He213 Chromosphere, models (dpeaa)DE-He213 Heating, chromospheric (dpeaa)DE-He213 Heating, in flares (dpeaa)DE-He213 Raulin, J.-P. verfasserin aut Mackinnon, A. verfasserin aut Giménez de Castro, G. verfasserin aut Simões, P. J. A. verfasserin aut Cabezas, D. verfasserin aut de La Luz, V. verfasserin aut Luoni, M. verfasserin aut Kaufmann, P. verfasserin aut Enthalten in Solar physics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967 290(2015), 10 vom: Okt., Seite 2809-2826 (DE-627)269019162 (DE-600)1473830-2 1573-093X nnns volume:290 year:2015 number:10 month:10 pages:2809-2826 https://dx.doi.org/10.1007/s11207-015-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 39.51 ASE AR 290 2015 10 10 2809-2826 |
allfieldsSound |
10.1007/s11207-015-0782-0 doi (DE-627)SPR017767180 (SPR)s11207-015-0782-0-e DE-627 ger DE-627 rakwb eng 530 ASE 39.51 bkl Trottet, G. verfasserin aut Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation. Radio bursts, microwave (dpeaa)DE-He213 X-ray bursts, association with flares (dpeaa)DE-He213 X-ray burst, spectrum (dpeaa)DE-He213 Chromosphere, models (dpeaa)DE-He213 Heating, chromospheric (dpeaa)DE-He213 Heating, in flares (dpeaa)DE-He213 Raulin, J.-P. verfasserin aut Mackinnon, A. verfasserin aut Giménez de Castro, G. verfasserin aut Simões, P. J. A. verfasserin aut Cabezas, D. verfasserin aut de La Luz, V. verfasserin aut Luoni, M. verfasserin aut Kaufmann, P. verfasserin aut Enthalten in Solar physics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967 290(2015), 10 vom: Okt., Seite 2809-2826 (DE-627)269019162 (DE-600)1473830-2 1573-093X nnns volume:290 year:2015 number:10 month:10 pages:2809-2826 https://dx.doi.org/10.1007/s11207-015-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 39.51 ASE AR 290 2015 10 10 2809-2826 |
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Enthalten in Solar physics 290(2015), 10 vom: Okt., Seite 2809-2826 volume:290 year:2015 number:10 month:10 pages:2809-2826 |
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Trottet, G. @@aut@@ Raulin, J.-P. @@aut@@ Mackinnon, A. @@aut@@ Giménez de Castro, G. @@aut@@ Simões, P. J. A. @@aut@@ Cabezas, D. @@aut@@ de La Luz, V. @@aut@@ Luoni, M. @@aut@@ Kaufmann, P. @@aut@@ |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR017767180</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111053536.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2015 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11207-015-0782-0</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR017767180</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s11207-015-0782-0-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">39.51</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Trottet, G.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2015</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Radio bursts, microwave</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">X-ray bursts, association with flares</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">X-ray burst, spectrum</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Chromosphere, models</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Heating, chromospheric</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Heating, in flares</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Raulin, J.-P.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Mackinnon, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Giménez de Castro, G.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Simões, P. 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|
author |
Trottet, G. |
spellingShingle |
Trottet, G. ddc 530 bkl 39.51 misc Radio bursts, microwave misc X-ray bursts, association with flares misc X-ray burst, spectrum misc Chromosphere, models misc Heating, chromospheric misc Heating, in flares Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT |
authorStr |
Trottet, G. |
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@@773@@(DE-627)269019162 |
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electronic Article |
dewey-ones |
530 - Physics |
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keep |
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aut aut aut aut aut aut aut aut aut |
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springer |
remote_str |
true |
illustrated |
Not Illustrated |
issn |
1573-093X |
topic_title |
530 ASE 39.51 bkl Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT Radio bursts, microwave (dpeaa)DE-He213 X-ray bursts, association with flares (dpeaa)DE-He213 X-ray burst, spectrum (dpeaa)DE-He213 Chromosphere, models (dpeaa)DE-He213 Heating, chromospheric (dpeaa)DE-He213 Heating, in flares (dpeaa)DE-He213 |
topic |
ddc 530 bkl 39.51 misc Radio bursts, microwave misc X-ray bursts, association with flares misc X-ray burst, spectrum misc Chromosphere, models misc Heating, chromospheric misc Heating, in flares |
topic_unstemmed |
ddc 530 bkl 39.51 misc Radio bursts, microwave misc X-ray bursts, association with flares misc X-ray burst, spectrum misc Chromosphere, models misc Heating, chromospheric misc Heating, in flares |
topic_browse |
ddc 530 bkl 39.51 misc Radio bursts, microwave misc X-ray bursts, association with flares misc X-ray burst, spectrum misc Chromosphere, models misc Heating, chromospheric misc Heating, in flares |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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Text Zeitschrift/Artikel |
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cr |
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Solar physics |
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Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT |
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Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT |
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Trottet, G. |
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Trottet, G. Raulin, J.-P. Mackinnon, A. Giménez de Castro, G. Simões, P. J. A. Cabezas, D. de La Luz, V. Luoni, M. Kaufmann, P. |
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origin of the 30 thz emission detected during the solar flare on 2012 march 13 at 17:20 ut |
title_auth |
Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT |
abstract |
Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation. |
abstractGer |
Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation. |
abstract_unstemmed |
Abstract Solar observations in the infrared domain can bring important clues on the response of the low solar atmosphere to primary energy released during flares. At present, the infrared continuum has been detected at 30 THz (10 μm) in only a few flares. SOL2012-03-13, which is one of these flares, has been presented and discussed in Kaufmann et al. (Astrophys. J.768, 134, 2013). No firm conclusions were drawn on the origin of the mid-infrared radiation. In this work we present a detailed multi-frequency analysis of the SOL2012-03-13 event, including observations at radio-millimeter and submillimeter wavelengths, in hard X-rays (HXR), gamma-rays (GR), $\mathrm{H}\alpha$, and white light. The HXR/GR spectral analysis shows that SOL2012-03-13 is a GR line flare and allows estimating the numbers of and energy contents in electrons, protons, and $\alpha$ particles produced during the flare. The energy spectrum of the electrons producing the HXR/GR continuum is consistent with a broken power-law with an energy break at ${\sim}\,800~\mbox{keV}$. We show that the high-energy part (above ${\sim}\, 800~\mbox{keV}$) of this distribution is responsible for the high-frequency radio emission (${>}\, 20~\mbox{GHz}$) detected during the flare. By comparing the 30 THz emission expected from semi-empirical and time-independent models of the quiet and flare atmospheres, we find that most (${\sim}\,80~\%$) of the observed 30 THz radiation can be attributed to thermal free–free emission of an optically thin source. Using the F2 flare atmospheric model (Machado et al. in Astrophys. J.242, 336, 1980), this thin source is found to be at temperatures T ${\sim}\,8000~\mbox{K}$ and is located well above the minimum temperature region. We argue that the chromospheric heating, which results in 80 % of the 30 THz excess radiation, can be due to energy deposition by nonthermal flare-accelerated electrons, protons, and $\alpha$ particles. The remaining 20 % of the 30 THz excess emission is found to be radiated from an optically thick atmospheric layer at T ${\sim}\, 5000~\mbox{K}$, below the temperature minimum region, where direct heating by nonthermal particles is insufficient to account for the observed infrared radiation. |
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Origin of the 30 THz Emission Detected During the Solar Flare on 2012 March 13 at 17:20 UT |
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score |
7.3985195 |