Solar Gamma-Ray Evidence for a Distinct Population of >1 MeV Flare-accelerated Electrons

Gerald H. Share, Ronald J. Murphy, Brian R. Dennis and Justin D. Finke
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Abstract

Significant improvements in our understanding of nuclear γ-ray line production and instrument performance allow us to better characterize the continuum emission from electrons at energies ≳300 keV during solar flares. We represent this emission by the sum of a power-law (PL) extension of hard X-rays and a power law times an exponential function (PLexp). We fit the γ-ray spectra in 25 large flares observed over 40 yr with this continuum and the calculated spectra of all known nuclear components. The PLexp is separated spectroscopically from the other components, and its presence is required with >99% confidence in 18 of the flares. Its distinct origin is suggested by significant differences between its time histories and those of the PL and nuclear components in 18 of the flares. RHESSI imaging/spectroscopy of the 2005 January 20 flare reveals that the PL and nuclear components come from the footpoints, while the PLexp component comes from the corona. While the index and flux of the anisotropic PL component are dependent on the flare’s heliocentric angle, the PLexp parameters do not show comparable dependences with 99.5% confidence. The PLexp spectrum is flat at low energies and rolls over at a few megaelectronvolts (MeV). Such a shape can be produced by thin-target bremsstrahlung from electrons with a spectrum that peaks between 3 and 5 MeV and by inverse Compton scattering of soft X-rays by 10–20 MeV electrons, or by a combination of the two. These electrons can produce radiation detectable at other wavelengths.
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太阳伽玛射线证据表明,存在bbbb1mev的耀斑加速电子
我们对核γ射线线产生和仪器性能的理解有了重大的改进,使我们能够更好地表征太阳耀斑期间能量为300kev的电子连续发射。我们用硬x射线的幂律(PL)扩展和幂律乘以指数函数(PLexp)的总和来表示这种发射。我们将40多年来观测到的25个大耀斑的γ射线谱与这个连续体和所有已知核成分的计算谱进行了拟合。PLexp在光谱上与其他成分分离,并且在18个耀斑中有99%的置信度需要它的存在。在18个耀斑中,其时间历史与PL和核成分的时间历史存在显著差异,这表明其独特的起源。2005年1月20日耀斑的RHESSI成像/光谱显示,PL和核成分来自足点,而PLexp成分来自日冕。虽然各向异性PL分量的指数和通量依赖于耀斑的日心角,但PLexp参数没有显示出可比较的相关性,可信度为99.5%。PLexp光谱在低能时是平坦的,在几兆电子伏特(MeV)时就会翻转。这种形状可以通过对峰值在3到5 MeV之间的电子进行薄靶轫致辐射,也可以通过10-20 MeV的电子对软x射线进行逆康普顿散射,或者两者的结合来产生。这些电子可以产生其他波长的辐射。
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