论文标题
在选定的时期中对MRK \,421的迅速观察。 iii。极端X射线正时/光谱属性和2015年12月至2018年的多波大处量态性
Swift observations of Mrk\,421 in selected epochs. iii. Extreme x-ray timing/spectral properties and multiwavelength lognormality in 2015\,December--2018\,April
论文作者
论文摘要
我们介绍了MRK \ \,421的定时和光谱研究的结果,主要基于\ emph {swift}数据在2015年时间间隔\ 2015年12月 - 2018年12月 - 2018年4月的X射线能量范围内。在2个月的时间内观察到了长期,每日和盘中时间尺度上最极端的X射线耀斑活动,该活动始于2017年\ 12月,当时0.3---10 \,Kev Flux超过5 $ \ times $ 10 $^{ - 9} $ 10 $^{ - 9} $ erg \ erg \,CM $^,CM $^{ - 2} $ s $ s $ s $ s $ s $^$ 1}尽管TEV波段和X射线变化大部分是相关的,但源通常在MEV(GEV和无线电)中以复杂的方式变化,UV能量范围,表明MRK \,421的多频发射不能总是在单个区域中产生。 X射线和$γ$砂的长期耀斑显示出对数正态特征,可能表明吸积盘的可变性在喷气机上。在0.3--10 \中,绝大多数KEV光谱与对数促羟基模型一致,在第一阶和二阶Fermi过程中预测的不同光谱参数之间的光谱曲率相对较低和相关性。 The position of the synchrotron spectral energy distribution (SED) peak showed an extreme variability on diverse timescales between the energies $E_{\rm p}$$<$0.1\,keV and $E_{\rm p}$$>$15\,keV, with 15\% of the spectra peaking at hard X-rays and was related to the peak height as $S_{\rm p} $$ \ varpropto $$ e^α_ {\ rm p} $带有$α$$ \ sim $ 0.6,这对于从kraichnan型湍流过渡到\ togequotedblleflleft hard-shard-phere \ thefere \ togequotedblright〜一个。 0.3--300 \ GEV光谱显示了在不同的时间间隔中,在克莱因 - 北山脉制度中,在克莱恩 - 北山智能中显示了hr子贡献的特征,喷气明星相互作用和向上散射。
We present the results from the timing and spectral study of Mrk\,421 based mainly on the \emph{Swift} data in the X-ray energy range obtained during the time interval 2015\,December--2018\,April. The most extreme X-ray flaring activity on the long-term, daily and intraday timescales was observed during the 2-month period which started in 2017\,December when the 0.3--10\,keV flux exceeded a level of 5$\times$10$^{-9}$erg\,cm$^{-2}$s$^{-1}$, recorded only twice previously. While the TeV-band and X-ray variabilities mostly were correlated, the source often varied in a complex manner in the MeV--GeV and radio--UV energy ranges, indicating that the multifrequency emission of Mrk\,421 could not be always generated in a single zone. The longer-term flares at X-rays and $γ$-rays showed a lognormal character, possibly indicating a variability imprint of the accretion disk onto the jet. A vast majority of the 0.3--10\,keV spectra were consistent with the log-parabolic model, showing relatively low spectral curvature and correlations between the different spectral parameters, predicted in the case of the first and second-order Fermi processes. The position of the synchrotron spectral energy distribution (SED) peak showed an extreme variability on diverse timescales between the energies $E_{\rm p}$$<$0.1\,keV and $E_{\rm p}$$>$15\,keV, with 15\% of the spectra peaking at hard X-rays and was related to the peak height as $S_{\rm p}$$\varpropto$$E^α_{\rm p}$ with $α$$\sim$0.6, which is expected for the transition from Kraichnan-type turbulence into the \textquotedblleft hard-sphere\textquotedblright~ one. The 0.3--300\,GeV spectra showed the features of the hadronic contribution, jet-star interaction and upscatter in the Klein-Nishina regime in different time intervals.