48个agn的22 ghz和37GHz爆发之间的时间滞后

W. Deng, J. Bai, Li Zhang, Xian Yang
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引用次数: 3

摘要

基于Metsahovi监测项目的22 GHz和37 GHz的光曲线,我们研究了48个无线电大agn的两个无线电频段之间的时间滞后。对数据进行了DCF和ZDCF分析。我们的研究结果表明,所有光源的两个无线电频率之间存在很强的相关性,在37 GHz的光曲线变化通常领先于22 GHz的光曲线。不同子类agn在时滞方面无明显差异。在两个源中,发现低频的爆发先于高频的爆发。一种可能的解释是,在辐射达到最大值之前,电子加速度主导着光曲线。一些源,如3C 273、3C 279、3C 345和3C 454.3,有足够好的数据,所以我们可以计算它们的滞后。我们的计算表明,不同的爆发有不同的滞后。有些脉冲具有正滞后,大多数脉冲没有明显滞后,少数脉冲具有负滞后。这一结果意味着不同的爆发是由不同的机制触发的,对这一结果的解释既包括内在机制,也包括几何机制。正滞后与激波模型很好地吻合,我们利用这些滞后来计算辐射区域的典型磁场强度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Time Lags between the 22 and 37GHz Bursts of 48 Radio-loud AGNs
Based on the light curves at 22 and 37 GHz from the Metsahovi monitoring program, we investigate the time lags between the two radio bands for 48 radio-loud AGNs. DCF and ZDCF analyses are applied to the data. Our results show that there is a strong correlation between the two radio frequencies for all the sources, with the variations in the light curves at 37 GHz leading the ones at 22 GHz in general. There is no obvious differences between different sub-class AGNs as regards the time lag. In two sources, it was found that the bursts at the lower frequency lead the ones at the higher frequency. One possible explanation is that electron acceleration dominates the light curve until the radiation reaches the maximum. Some sources, such as 3C 273, 3C 279, 3C 345 and 3C 454.3, have good enough data, so we can calculate their lags burst-by-burst. Our calculations show that different outbursts have different lags. Some bursts have positive lags, most of bursts have no clear lags, and a few have negative lags. This result means that different bursts are triggered by different mechanisms, and the interpretation for the result involves both an intrinsic and a geometric mechanism. The positive lags are well consistent with the shock model, and we use these lags to calculate the typical magnetic field strength of the radiating region.
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