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Plasma effects on fast pair beams II. Reactive versus kinetic instability of parallel electrostatic wave

机译:等离子体对快速双光束的影响II。反应性与动力学   并联静电波的不稳定性

摘要

The interaction of TeV gamma rays from distant blazars with the extragalacticbackground light produces relativistic electron-positron pair beams by thephoton-photon annihilation process. Using the linear instability analysis inthe kinetic limit, which properly accounts for the longitudinal and the smallbut finite perpendicular momentum spread in the pair momentum distributionfunction, the growth rate of parallel propagating electrostatic oscillations inthe intergalactic medium is calculated. Contrary to the claims of Miniati andElyiv (2013) we find that neither the longitudinal nor the perpendicular spreadin the relativistic pair distribution function do significantly affect theelectrostatic growth rates. The maximum kinetic growth rate for noperpendicular spread is even about an order of magnitude greater than thecorresponding reactive maximum growth rate. The reduction factors to themaximum growth rate due to the finite perpendicular spread in the pairdistribution function are tiny, and always less than $10^{-4}$. We confirm theearlier conclusions by Broderick et al. (2012) and us, that the created pairbeam distribution function is quickly unstable in the unmagnetizedintergalactic medium. Therefore, there is no need to require the existence ofsmall intergalactic magnetic fields to scatter the produced pairs, so that theexplanation (made by several authors) of the FERMI non-detection of the inverseCompton scattered GeV gamma rays by a finite deflecting intergalactic magneticfield is not necessary. In particular, the various derived lower bounds for theintergalactic magnetic fields are invalid due to the pair beam instabilityargument.
机译:来自远处的天体的TeV伽马射线与银河外背景光的相互作用通过光子-光子an灭过程产生了相对论的电子-正电子对束。使用动力学极限中的线性不稳定性分析(适当地考虑了对动量分布函数中的纵向动量和有限的垂直动量散布),计算了星际介质中平行传播的静电振荡的增长率。与Miniati和Elyiv(2013)的观点相反,我们发现相对论对分布函数中的纵向扩展和垂直扩展都不会显着影响静电增长率。非垂直扩散的最大动力学增长率甚至比相应的反应性最大增长率大一个数量级。由于成对分布函数中的垂直分布有限,导致最大增长率的减小因子很小,并且总是小于$ 10 ^ {-4} $。我们证实了Broderick等人的早期结论。 (2012)和我们,在非磁化星系间介质中,所创建的成对光束分布函数很快不稳定。因此,无需要求存在较小的星际磁场来散射产生的星对,因此,由有限偏转星际磁场对费米未检测到的反康普顿散射GeV伽马射线的FERMI的解释(由几位作者进行)必要。尤其是,由于成对的电子束不稳定性参数,导致星系间磁场的各种导出下限无效。

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