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Quasi-linear stage of synchrotron instability. II. Monoenergetic initial electron distribution

机译:同步加速器不稳定的准线性阶段。二。单能初始电子分布

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Using the results obtained in the first part of the work, we analyze quasi-linear relaxation of an initial monoenergetic quasi-isotropic electron distribution embedded in a cold plasma. It is shown that in this case the radiation energy density increases due to synchrotron instability only at the initial stage of relaxation and after that reabsorption emerges. At the stage of reabsorption, electrons absorb the emitted radiation for the same characteristic time as the time of radiation energy density increase at the maser stage. We calculate the maximum fraction of initial electron energy which is converted into synchrotron radiation energy. Analytical expressions are obtained for the amplitude and width of the frequency spectrum at the instant of the maximum level of synchrotron radiation and for the maximum value and width of the electron distribution over momentum at the end of relaxation.
机译:使用在工作的第一部分中获得的结果,我们分析了嵌入在冷等离子体中的初始单能准各向同性电子分布的准线性弛豫。结果表明,在这种情况下,辐射能量密度仅由于同步加速器的不稳定性而增加,仅在弛豫的初始阶段和之后才出现重吸收。在再吸收阶段,电子吸收发射的辐射的时间与maser阶段辐射能量密度增加的时间相同。我们计算初始电子能量的最大分数,该分数将转换为同步加速器辐射能。在同步加速器辐射达到最大水平时获得频谱的幅度和宽度,在弛豫结束时获得动量上电子分布的最大值和宽度的解析表达式。

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